CN117492059A

CN117492059A - Substance component determining method and device, electronic apparatus, and storage medium

Info

Publication number: CN117492059A
Application number: CN202311526718.XA
Authority: CN
Inventors: 谢庆国; 吕旭东; 华越轩; 肖鹏; 李硕; 龚正光; 凌怡清; 邱奥
Original assignee: Raycan Technology Co Ltd
Current assignee: Raycan Technology Co Ltd
Priority date: 2023-11-16
Filing date: 2023-11-16
Publication date: 2024-02-02

Abstract

The application discloses a substance component determining method and device, an electronic device and a storage medium. The substance component determining method comprises the following steps: providing amplitude-energy mapping relationship data of a reference scintillation pulse generated by high-energy rays; determining an energy window of at least one component in the substance to be detected, which corresponds to the high-energy ray; determining a scintillation pulse amplitude range corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window; determining the count of the scintillation pulses to be detected falling into the amplitude range according to the comparison of the amplitude of a plurality of scintillation pulses to be detected generated by detecting the high-energy rays emitted by the substances to be detected and the amplitude range; and determining the content of the at least one component of the substance to be tested according to the count. The method avoids complex fitting calculation, overcomes the defect that the traditional mode is intolerant to high temperature, directly analyzes and judges the content of the substance components through a concise threshold comparison mode, and has high sampling rate and high working stability.

Description

Substance component determining method and device, electronic apparatus, and storage medium

Technical Field

The present invention relates to the field of signal sampling, and in particular, to a method and apparatus for determining a substance component, an electronic device, and a storage medium.

Background

In many applications of high-energy ray detection, high-energy rays, such as gamma rays, are converted into visible light by a scintillation crystal, which is further converted into a scintillation pulse signal by a photoelectric conversion device.

The logging technology is an important technical means in the petroleum exploration field, and can combine electronic technology and computer technology together through various modes such as electricity, acoustics, radiology and the like to acquire various physical parameters of stratum, and further acquire oil and gas information through data analysis. Common logging techniques include electrical logging, sonic logging, nuclear magnetic logging, and the like. Nuclear logging is based on the nuclear physical properties of substances, and drilling geological sections are researched according to the nuclear physical properties of rock, pore fluid and medium in the well, so as to search for mineral reservoirs such as coal, petroleum and the like. Nuclear logging uses high-energy ray detection, and uses logging techniques such as natural gamma, density, neutrons, stratum elements and the like and matched instruments.

The pulse neutron well logging method is one of nuclear well logging, and is based on the principle that energy of pulse neutrons is acquired and deposited in stratum to release gamma rays so as to acquire corresponding energy spectrum information and time spectrum information. The main means of high-energy ray detection is to use a scintillation crystal to couple with a photoelectric conversion device, and the energy of the high-energy ray deposited by the scintillation crystal is used for generating visible light and converted into an electric signal by the photoelectric conversion device to obtain information such as the energy of the high-energy ray. Currently, a photomultiplier tube that can operate at a high temperature is generally used as a photoelectric conversion device to convert visible light generated by a scintillation crystal into a corresponding scintillation pulse, and energy information (such as an energy spectrum) and time information (such as a time spectrum) of gamma rays obtained after digitization and subsequent signal processing are correspondingly obtained, and components of a logging substance, such as a carbon-oxygen ratio C/O, can be determined according to the energy information of gamma rays.

There are two conventional methods of obtaining the scintillator composition. One is a method of direct digitization of a high-speed ADC, which requires first shaping and stretching the electrical pulse signal, and then digitally sampling using the high-speed ADC (e.g., 1 GSps). Typically, to obtain relatively accurate energy information, it is necessary in engineering practice to digitize a pulse by taking multiple (e.g., 20) sampling points while operating at high temperature (e.g., 175 ℃). However, the sampling rate performance of the ADC chip at this high temperature is generally not high, and the cost is high, so it is difficult to digitize the high-speed scintillation pulse signal, making the direct digitizing method of the high-speed ADC more difficult to apply to petroleum logging. Another is the peak hold method, which uses a peak hold circuit to lock the amplitude of the electrical pulse signal and then uses an ADC to collect the amplitude to obtain energy information of the pulse. Peak hold methods have peak hold lock set-up and peak hold circuit recovery processes that have long dead times, typically on the order of hundreds of microseconds, which greatly limits the rate of digitized pulses (the number of pulses processed per unit time). In oil logging, the number of pulse events often increases in bursts. For example, in a typical neutron oil well logging, the number of pulses would reach 100KCPS, with an average of one pulse per 10 μs. Dead time of the peak hold method can cause the digitizing process to lose many pulse signals, thereby causing measurement bias.

In recent years, the method for directly digitizing scintillation pulses and replacing the traditional analog circuit with a software algorithm to extract information has great development potential. A Multi-voltage threshold sampling (MVT) method is proposed as an improved digital processing method of the scintillation pulse. Currently, the introduction of MVT digitization methods into the field of oil exploration is also proposed.

Compared with the traditional ADC time interval sampling method, the MVT digital sampling method has the advantages that a plurality of threshold voltages are fixed, and the time when the scintillation pulse passes through the threshold voltages is digitally sampled, so that a plurality of sampling points can be acquired in a rapid rising edge stage. In specific practice, after a series of time-voltage pair information is obtained, accurate acquisition of particle energy deposition information is achieved by a pulse fitting method. For example, the Levenberg-Marquardt (Levenberg-Marquardt) method, which is a widely used nonlinear least squares iterative algorithm, is a nonlinear optimization method that uses gradients to find maximum (small) values, between newton's method and gradient descent method, and has the advantages of both gradient method and newton's method, can be generally used as the pulse fitting optimization algorithm.

However, due to the excessive complexity of chip computing power and fitting methods, the MVT-based fitting algorithm cannot be implemented in embedded chips such as FPGAs, STMs 32, DSPs, and the like, and accessories thereof, which limits the possibility of implementing MVT-based fitting algorithms in the field (on site), such as a detection well. Therefore, the original sampling points obtained by the MVT method are transmitted to computer equipment (also called an upper computer) with stronger calculation power far away from the site in a remote communication mode such as Ethernet, serial ports, wiFi and the like, and the energy is calculated by an iterative algorithm. In the petroleum well logging process, the flash pulse generation time shows the characteristic of periodic burst, and the data volume of an original sampling point is extremely large, for example, the data volume can reach 10Mbps to 1Gbps. In addition, the method is limited in the use scene of petroleum detection, has the characteristics of high downhole depth up to ten thousand meters and high environmental temperature, has a limited transmission mode, can only adopt a carrier communication mode for transmission, and has a bandwidth of only about 100 Kbps. The current method causes contradiction that the data quantity of the original sampling point is relatively large and the transmission bandwidth is relatively small, so that the counting rate is reduced. Furthermore, fitting on a host computer requires an ultra high CPU time for each pulse to fit because of repeated iterations, which is intolerable in using oil exploration.

In addition, the current MVT method may have several drawbacks in acquiring energy information of the scintillation pulse, for example, the conventional MVT method is suitable for acquiring a pulse of a known type, and the setting of the threshold value is determined according to the energy range of the known pulse. Accordingly, the MVT method requires selecting a fixed number and size of thresholds for sampling. Thus, conventional MVT methods generally can only obtain more accurate energy information for pulses within a certain energy range.

Since MVT requires fitting to calculate accurate energy values, accurate time information needs to be provided for each data point. For this reason, a large number of TDCs (clock digitizers) are generally required to be employed in the acquisition circuit to acquire time information.

In addition, pulse fitting is performed on hardware circuits such as an FPGA, an ASIC and the like, and it is necessary to restore the pulse waveform first, then integrate the fitted function to calculate energy information, and then draw an energy spectrum. However, complex computing processes will occupy a significant amount of hardware resources and increase the power consumption of the hardware circuitry. For application scenes such as logging equipment, which need to be suitable for high-temperature environments, the hardware circuit power consumption caused by the excessively complex pulse fitting and integration process is too large, and the high-temperature resistance of the hardware circuit can be further affected.

It is therefore desirable to provide a solution that can quickly determine the content of a substance component by quickly, accurately and stably acquiring information about a scintillation pulse signal generated based on a high-energy radiation detecting substance, and that is suitable for implementation in a hardware circuit such as an FPGA, DSP, etc., without consuming a large amount of computing resources or using a computer device with a strong computing power.

The description of the background art is only for the purpose of facilitating an understanding of the relevant art and is not to be taken as an admission of the prior art.

Disclosure of Invention

The technical problem to be solved by the embodiments of the present application is to provide a material component content determination scheme of scintillation pulse generated based on high-energy ray detection material, which is suitable for implementation in hardware circuits such as FPGA, DSP, etc., and can avoid complex fitting calculation required by the traditional method for acquiring pulse, especially scintillation pulse energy information.

In order to solve the problems, the application discloses a substance component determining method and device, an electronic device and a storage medium.

In a first aspect, there is provided a substance constituent determining method comprising:

providing amplitude-energy mapping relationship data of a reference scintillation pulse generated by high-energy rays;

determining an energy window of at least one component in the substance to be detected, which corresponds to the high-energy ray;

Determining a scintillation pulse amplitude range corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window;

determining the count of the scintillation pulses to be detected falling into the amplitude range according to the comparison of the amplitude of a plurality of scintillation pulses to be detected generated by detecting the high-energy rays emitted by the substances to be detected and the amplitude range; and

determining the content of the at least one component of the substance to be tested based on the count.

In a second aspect, there is provided a substance constituent determining method comprising:

setting a plurality of addresses, wherein the addresses are energy addresses or amplitude addresses, each energy address has a respective energy representation value and a corresponding amplitude representation value determined according to the amplitude-energy mapping relation data, and each amplitude address has a respective amplitude representation value;

determining the channel addresses corresponding to the scintillation pulses to be detected according to the comparison of the amplitude values of the scintillation pulses to be detected and the amplitude characterization values of the channel addresses, wherein the scintillation pulses to be detected are generated by detecting high-energy rays emitted by substances to be detected;

determining a track address interval corresponding to the energy window based on the amplitude-energy mapping relation data and the energy window; and

and determining the content of the at least one component of the substance to be detected according to the scintillation pulse count to be detected in each channel address and the determined channel address interval.

In a third aspect, there is provided a substance component determining apparatus comprising:

the mapping relation database comprises amplitude-energy mapping relation data of reference scintillation pulse generated by high-energy rays;

an energy window determining unit configured to determine an energy window of at least one component in the substance to be measured corresponding to the high-energy ray;

an amplitude range determining unit configured to determine a scintillation pulse amplitude range corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window;

the counting unit is configured to determine the count of the scintillation pulses to be detected falling into the amplitude range according to the comparison of the amplitude of the scintillation pulses to be detected generated by detecting the high-energy rays emitted by the substances to be detected and the amplitude range; and

and a content determining unit configured to determine a content of the at least one component of the substance to be measured based on the count.

In a fourth aspect, there is provided a substance component determining apparatus comprising:

an address setting unit configured to set a plurality of addresses, wherein the addresses are energy addresses or amplitude addresses, each energy address has a respective energy characterization value and a magnitude characterization value determined correspondingly according to the magnitude-energy mapping relationship data, and each amplitude address has a respective magnitude characterization value;

the channel address determining unit is configured to determine channel addresses corresponding to a plurality of scintillation pulses to be detected according to comparison of the amplitude values of the scintillation pulses to be detected and the amplitude representation values of the channel addresses, wherein the scintillation pulses to be detected are generated by detecting high-energy rays emitted by a substance to be detected;

a track address section determining unit configured to determine a track address section corresponding to the energy window based on the amplitude-energy mapping relation data and the energy window; and

and a content determining unit configured to determine a content of the at least one component of the substance to be measured based on the count of scintillation pulses to be measured in each of the addresses and the determined address range.

In a fifth aspect, there is provided an electronic device, comprising: a memory, a processor and an executable program stored on the memory and executable on the processor, which when executed by the processor, implements the steps of the method according to any of the embodiments of the present application.

In a sixth aspect, a storage medium is provided, characterized in that the storage medium has stored thereon an executable program, which when executed by a processor, implements the steps of the method according to any of the embodiments of the present application.

In other aspects of the application, methods, apparatus, devices for digitizing a pulse signal and correction methods and apparatus suitable for digitizing the pulse are also provided.

Optional features and other effects of embodiments of the present application are described in part below, and in part will be apparent from reading the disclosure herein.

Drawings

In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings that are required to be used in the embodiments or the description of the prior art will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments described in the present invention, and other drawings may be obtained according to the drawings without inventive effort to those skilled in the art.

FIG. 1 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 2 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 3 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 4 shows a first block architecture diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 5 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 6 shows a second module architecture diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 7 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 8 shows a third block diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 9 is a schematic diagram showing the determination of the energy addresses corresponding to pulse amplitudes by a dichotomy multi-level comparison in a material composition acquisition method according to an embodiment of the present application;

FIG. 10 shows a fourth block diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 11 illustrates a pulse schematic diagram of determining amplitude using a quartering multi-level comparison in a material composition acquisition method according to an embodiment of the present application, particularly illustrating a first level comparison;

FIG. 12 shows a fifth block diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 13 shows a sixth block architecture diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 14 shows a seventh block diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 15 shows an eighth block architecture diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 16 shows a ninth block diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 17 shows a tenth module architecture diagram for implementing a substance constituent acquisition method according to an embodiment of the present application;

FIG. 18 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 19 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 20 shows an eleventh block architecture diagram for implementing a material composition acquisition method according to an embodiment of the present application;

FIG. 21 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 22 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 23 shows a twelfth module architecture diagram for implementing a substance constituent acquisition method according to an embodiment of the present application;

FIG. 24 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 25 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 26 shows a thirteenth block diagram for implementing a substance constituent acquisition method according to an embodiment of the present application;

FIG. 27 is a diagram showing the threshold time TOT of a pulse under test and the transition signal used to determine TOT;

FIG. 28 shows a fourteenth block architecture diagram for implementing a substance constituent acquisition method according to an embodiment of the present application;

FIG. 29 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 30 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 31 illustrates an exemplary flow chart of a method of substance constituent acquisition according to an embodiment of the present application;

FIG. 32 illustrates an exemplary flow chart of a correction method for pulse digitization according to an embodiment of the present application;

FIG. 33 illustrates an exemplary flow chart of a scintillation pulse-based material composition determination method in accordance with an embodiment of the present application;

FIG. 34 illustrates an exemplary flow chart of a scintillation pulse-based material composition determination method in accordance with an embodiment of the present application;

FIG. 35 shows a schematic block diagram of a pulse digitizing apparatus according to an embodiment of the application;

FIG. 36 shows a schematic block diagram of a correction device for pulse digitization according to an embodiment of the present application;

FIG. 37 shows a schematic block diagram of a scintillation pulse-based material composition determination apparatus in accordance with an embodiment of the present application;

fig. 38 shows a schematic block diagram of a scintillation pulse-based substance constituent determining apparatus in accordance with an embodiment of the present application.

Description of the embodiments

In order to make the above objects, features and advantages of the present application more comprehensible, embodiments accompanied with figures are described in detail below. In the following description, numerous specific details are set forth in order to provide a thorough understanding of the present application. This application is, however, susceptible of embodiment in many other forms than those described herein and similar modifications can be made by those skilled in the art without departing from the spirit of the application, and therefore the application is not to be limited to the specific embodiments disclosed below.

It will be understood that when an element is referred to as being "fixed to" another element, it can be directly on the other element or intervening elements may also be present. When an element is referred to as being "connected" to another element, it can be directly connected to the other element or intervening elements may also be present. The terms "vertical," "horizontal," "left," "right," and the like are used herein for illustrative purposes only. The described features, structures, or characteristics may be combined in any suitable manner in one or more embodiments. In the following description, numerous specific details are provided to give a thorough understanding of embodiments of the present application. One skilled in the relevant art will recognize, however, that the aspects of the application can be practiced without one or more of the specific details, or with other methods, components, materials, devices, operations, etc. In these instances, well-known structures, methods, devices, implementations, materials, or operations are not shown or described in detail.

The flow diagrams depicted in the figures are exemplary only, and do not necessarily include all of the elements and operations/steps, nor must they be performed in the order described. For example, some operations/steps may be decomposed, and some operations/steps may be combined or partially combined, so that the order of actual execution may be changed according to actual situations.

The terms first, second and the like in the description and in the claims of the present application and in the above-described figures, are used for distinguishing between different objects and not for describing a particular sequential order. Furthermore, the terms "comprise" and "have," as well as any variations thereof, are intended to cover a non-exclusive inclusion. For example, a process, method, system, article, or apparatus that comprises a list of steps or elements is not limited to only those listed steps or elements but may include other steps or elements not listed or inherent to such process, method, article, or apparatus. The term "and/or" and/or "includes any and all combinations of one or more of the associated listed items.

Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs. The terminology used herein in the description of the application is for the purpose of describing particular embodiments only and is not intended to be limiting of the application.

Some preferred embodiments of the present application are described below with reference to the accompanying drawings. It should be noted that the following description is for illustrative purposes and is not intended to limit the scope of the present application.

FIG. 1 is an exemplary flow chart of a method of substance constituent acquisition according to some embodiments of the present application. In some embodiments, the substance constituent acquisition method 100 may be performed by a pulse digitizing apparatus, such as the pulse digitizing apparatus 3200 shown in fig. 32. In some embodiments, the substance constituent acquisition method 100 may be implemented in software, hardware, firmware, or a combination thereof. In some preferred embodiments, the substance constituent acquisition method 100 may be implemented by hardware-based circuitry, such as, for example, implementation in hardware-based circuitry such as FPGA, DSP, etc. In a preferred embodiment, the substance constituent obtaining method 100 may be implemented by an apparatus including an FPGA chip.

In this context, a pulse signal can be interpreted as any pulse signal that enables sampling, essentially a physical quantity that has a sudden change in a short time and then returns rapidly to its original value, the physical quantity having a certain characteristic.

In embodiments of the present application, pulse digitization may involve converting a pulse signal, for example in analog or physical form, into a numerical parameter that characterizes the pulse signal for subsequent reconstruction of the pulse signal image or other purposes related to processing, converting, transmitting the pulse signal. In a specific embodiment, pulse digitization may involve acquiring physical parameter information characterized by the pulse signal, and more particularly, energy information characterized by the pulse signal. Thus, in some embodiments herein, the substance constituent acquisition method may specifically relate to a pulse energy information determination method.

In embodiments of the present application, pulse digitization may be used in a number of applications for high energy ray detection. As previously mentioned, by way of explanation and not limitation, high energy rays, such as gamma rays, may be converted by the scintillation crystal into visible light, which is further converted by the photoelectric conversion device into a scintillation pulse signal. In embodiments of the present application, the pulse signal may include, inter alia, a scintillation pulse. Accordingly, in the embodiment of the present application, the substance component acquisition method may be a scintillator substance component acquisition method. Similarly, the pulse digitizing apparatus or device of embodiments of the application may be a scintillation pulse digitizing apparatus or device.

Various embodiments will be described herein, taking scintillation pulses as an example, in which the pulses and scintillation pulses may be interchanged. For example, in some embodiments, the scintillation pulse typically has a rising edge and a falling edge, and the rising edge and the falling edge can be represented by a functional model. For example, a scintillation pulse corresponding to a gamma photon typically exhibits a relatively fast rising edge, which may be characterized by a linear function, and a relatively slow falling edge, which may be characterized by an exponential function.

In some embodiments, the scintillation pulse may be acquired by a detector, such as a PET detector, a CT detector, a neutron detector, a petroleum detector, which typically include a scintillation crystal for converting detected high-energy rays (e.g., gamma rays, neutron rays, etc.) into a visible light signal, and a photoelectric conversion device (e.g., photomultiplier tube PMT, silicon photomultiplier tube SiPM, etc.) for converting the visible light signal into an electrical signal that is output in the form of a scintillation pulse signal through electronics coupled to the photoelectric conversion device.

Accordingly, the method, apparatus and/or device for obtaining a substance component according to embodiments of the present application may be used in a number of applications for high-energy ray detection based on energy information of a scintillation pulse signal. For example, the material composition acquisition methods, apparatus, and/or devices according to embodiments of the present application may be used in well logging employing high energy ray detection, such as nuclear well logging, more particularly pulsed neutron well logging. The method, the device and/or the equipment for acquiring the substance component can be used for acquiring energy information, such as energy spectrum, of gamma rays released by a pulse neutron well logging method. In addition, the method, apparatus and/or device for obtaining a substance component according to the embodiments of the present application may also be used in a variety of application fields where high-energy ray detection is used, such as, but not limited to, medical imaging technology, high-energy physics, laser radar, autopilot, precision analysis, optical communication, and the like. In a specific example, the substance component obtaining method, apparatus and/or device according to embodiments of the present application may be used in one of a Positron Emission Tomography (PET) device, a CT device, an MRI device, a radiation detection device, a petroleum detection device, a dim light detection device, a SPECT device, a security inspection device, a gamma camera, an X-ray device, a DR device, etc., or a combination of the above devices using the principle of high energy ray conversion.

In other embodiments, the pulse signal may be a non-blinking pulse, and the waveform of the pulse signal may be a triangular wave, a rectangular wave, a sine wave, a cosine wave, or some other shaped wave, which will not be described herein.

In the embodiment of the present application, the pulse signal expression form may be an electrical pulse signal, an acoustic pulse signal, a thermal pulse signal, or a pressure wave signal, for example, when the pulse signal is an electrical pulse signal, the corresponding characteristic may be a voltage or a current of the electrical pulse signal; when the pulse signal is an acoustic pulse signal, the corresponding characteristic may be the sound intensity of the acoustic pulse signal, and so on, which will not be described herein. Correspondingly, the threshold may have various manifestations, for example, when the pulse signal is an electric pulse signal, the corresponding threshold may be a voltage threshold, a current threshold or an energy threshold; when the pulse signal is an acoustic pulse signal, the corresponding threshold value may be a sound intensity threshold value, and so on, which will not be described herein.

It will be appreciated by those skilled in the art that pulse digitization in this application is also applicable to the digitization of a continuous signal, which need only be considered as a pulse signal arranged in a certain period. The pulse signal in this application is not to be taken as a limitation of the sampled signal.

With continued reference to fig. 1, a substance constituent acquisition method 100 according to an embodiment of the present application is described. In this embodiment of the present application, based on the correspondence between the energy of the pulse, such as the scintillation pulse, and the (maximum) amplitude, a plurality of amplitude addresses may be set for the pulse, such as the amplitude of the scintillation pulse, or a plurality of energy addresses may be set for the pulse, such as the energy of the scintillation pulse, and statistics may be performed on the number of pulses whose amplitude or energy corresponds to fall into different addresses to obtain energy information of the pulse, such as the scintillation pulse. In one particular embodiment, an energy distribution histogram may be drawn, for example, from pulse counts to obtain an energy spectrum (energy spectrum for short). For example, in a specific example, such as in pulse neutron saturation logging, for the energy characteristic (e.g., typically within 9 Mev) of the scintillation pulse corresponding to the gamma ray, the energy of the pulse may be quantized into N (e.g., 256) different levels to obtain N (e.g., 256) different energy addresses, and the number of pulses on the energy levels corresponding to the different energy addresses may be counted and plotted into an energy distribution histogram to obtain the energy spectrum of the scintillation pulse. Those skilled in the art will appreciate that 256 addresses will be described as an example in several embodiments described below, but other numbers (n+.256) of addresses are conceivable, which fall within the scope of the present application.

Specifically, as shown in fig. 1, the material composition acquisition method 100 may include step S110 of providing amplitude-energy mapping relationship data of a plurality of reference pulses.

In one embodiment, the providing amplitude-energy mapping relationship data of the plurality of reference pulses includes: providing an amplitude-energy look-up table of the plurality of reference pulses.

By collecting a priori information analysis, the inventors have found that there is a significant linear relationship between pulse energy and pulse (maximum) amplitude, whereby energy information of the pulse can be obtained indirectly by obtaining amplitude information of the pulse. Accordingly, in embodiments of the present application, a pulse, such as a scintillation pulse, amplitude-energy lookup table may be created based on pulse prior information, which may characterize the mapping between pulse amplitude and pulse energy.

In one embodiment, a collection device, such as an oscilloscope, may be used to collect a number of pulses, such as scintillation pulse data, and each pulse, such as scintillation pulse, may be integrated to obtain its energy value while recording the amplitude of the pulse. Thus, a number of reference pulses, such as reference scintillation pulses, can be obtained with respect to the correspondence between the energy and the pulse amplitude, and these a priori information can be used to create a pulse, such as scintillation pulse, amplitude-energy lookup table. In some embodiments, these reference pulses may be pulses that are homologous to the pulses under test. For example, when applied to nuclear logging to obtain energy information for a pulse under test, the reference pulse may be a scintillation pulse obtained from the same well or a similar well (e.g., a petroleum well) using the same source. In some embodiments these reference pulses may be pulses similar to the pulse under test. For example, when applied to nuclear logging to obtain energy information from a pulse under test, the reference pulse may be a scintillation pulse converted from the same or similar high energy rays, such as gamma rays, through a scintillation crystal, but the reference pulse is not from the same or a similar well or from a different type of well (e.g., other energy well).

Other flicker amplitude-energy mapping relationship data may be used in addition to or in place of the amplitude-energy lookup table. For example, a function that characterizes a simple linear relationship between pulse energy and pulse (maximum) amplitude may be used. The energy corresponding to the amplitude of at least part of the pulse to be measured can be obtained by simple linear interpolation based on the linear relation function.

In a further embodiment, the method 100 for obtaining a substance component may include step S120, setting a plurality of addresses.

In this context, the term "address" is a channel address that characterizes the pulse, e.g. the pulse characteristic value of a scintillation pulse. In embodiments of the present application, the plurality of addresses may collectively characterize a continuous range of characteristic values or separately characterize a plurality of sequential characteristic values, as will be further explained below.

In some embodiments, the addresses may be energy addresses, each energy address having a respective energy characterization value.

In the embodiment of the present application, step S120 may include: and determining energy representation values corresponding to all the energy addresses, and determining the pulse amplitude representation values corresponding to the energy representation values according to the amplitude-energy mapping relation data so as to set a plurality of energy addresses.

In the embodiment of the present application, the characteristic value may be interpreted broadly, and covers a characteristic value interval or a single characteristic value.

For example, in one embodiment, the energy addresses (e.g., the nth energy address, n being a natural number) may have their corresponding energy intervals [ E ] _n ，E _n+1 ) The energy interval is the energy sign value of the corresponding track address. Accordingly, multiple (e.g., N being a natural number) energy addresses may collectively characterize a larger continuous energy range [ E ₁ ，E _N ]。

In alternative embodiments, the energy addresses may have a single energy signature value corresponding thereto, e.gThe lower limit, the upper limit, the median value, etc. of the energy interval. For example, the energy characteristic value of the nth energy track is the energy interval [ E ] _n ，E _n+1 ) Lower limit E of (2) _n . Here, multiple (e.g., N) energy addresses may each represent multiple sequential energy values, e.g., E ₁ ，E ₂ ，……，E _N 。

Specifically, according to the energy information of the pulse to be detected and the energy address number determined according to the actual need, the energy interval or the single energy sign value corresponding to each energy address can be determined.

In this embodiment of the present application, each energy address further includes an amplitude characterizing value that is determined according to the amplitude-energy mapping relationship data.

Specifically, the respective amplitude characterizing values of the energy addresses may be determined based on the amplitude-energy mapping relation data provided in step S110, such as an amplitude-energy lookup table. Similarly, the amplitude characterization value may be a pulse amplitude (peak) interval or a single amplitude (peak) characterization value. Preferably, when the energy characteristic value is a zone, the amplitude characteristic value is also a zone. In this embodiment, the energy intervals of each energy track address may be correlated with the pulse amplitude (peak value) intervals according to a lookup table to obtain the respective pulse amplitude intervals of each energy track address.

In one embodiment, the total energy address number may be determined according to practical applications, and based on the provided energy amplitude lookup table of the scintillation pulse, different levels of energy (energy intervals) corresponding to different energy addresses are respectively corresponding to the pulse peak intervals, so that the energy addresses (energy intervals) correspond to the pulse peak intervals. In several embodiments described below, an exemplary total energy track number is 256 (n=256). However, those skilled in the art will appreciate that these embodiments may be practiced with other total numbers of addresses as desired.

Pulse amplitudes (peaks) in embodiments of the present application include, but are not limited to, current peaks, voltage peaks, and the like. In a further embodiment, the pulse amplitude (peak value) may include a voltage peak value, each energy track address corresponds toThe pulse voltage amplitude at a certain end point of the peak interval of (2) is respectively denoted as V ₁ ，V ₂ ，V ₃ … …. In several specific embodiments described below, the pulse voltage amplitude V at the end points will be based on ₁ ，V ₂ ，V ₃ … … determines whether the pulse under test falls within the associated energy trace, however, those skilled in the art will appreciate that these embodiments may determine whether the pulse under test falls within the associated energy trace at other types of pulse amplitudes, or at other values within a range (such as another endpoint or a range median) or based on a single amplitude characterization as previously described, as desired.

In some embodiments of the present application, the plurality of addresses are equally spaced, i.e., the ranges of intervals of the tokens are equal or the intervals of the sequential individual token values are equal. In a further embodiment, when the address is an energy address, the energy values may be equally spaced (strictly) or the amplitude values may be equally spaced (strictly) as well. For example, when the address is an energy address, the (single) energy value of each of the nth energy address is E _n (Single) amplitude characterization value V _n In some embodiments, E _n+2 -E _n+1 =E _n+1 -E _n The method comprises the steps of carrying out a first treatment on the surface of the In other embodiments, V _n+2 -V _n+1 =V _n+1 -V _n . It will be appreciated here that although there is a substantially linear relationship between pulse energy and pulse (maximum) amplitude, equally spaced energy addresses based on either energy or amplitude characterization values may be selected as desired, both of which fall within the scope of the present application.

It should be understood by those skilled in the art that the plurality of addresses may also be non-equally spaced, i.e., the ranges of the intervals of the characterizations are not exactly equal or all are not equal or the single values of the characterizations of the sequence are not exactly equal or all are not equal, as will be apparent to those skilled in the art from the teachings of the present application and will not be repeated here.

In further embodiments, the addresses may be amplitude addresses, each having a respective amplitude characterization value.

In this embodiment, the total number of total amplitude addresses may be set as required, or the amplitude range commonly represented by the plurality of amplitude addresses may be determined according to the prior information such as the reference pulse or other reference pulse described in step S110. Accordingly, the total number of the amplitude addresses and/or the amplitude representation value of each amplitude address can be set in a targeted manner according to the characteristics of the pulse to be detected, and in different pulse digitizing schemes, the total number of the amplitude addresses and/or the amplitude representation value of each amplitude address are different. However, in alternative embodiments, a fixed total number of amplitude addresses and a fixed amplitude characterization value may be provided for each of the different digitizing schemes, which fall within the scope of the present application. For example, the digitization schemes for the different pulses each provide a given total number N of amplitude addresses (e.g., n=256) and a given amplitude characterization value (e.g., each V ₁ ，V ₂ ，V ₃ ，……）。

In embodiments where multiple amplitude addresses are provided, the mapping between pulse amplitude and energy may not be considered. Accordingly, in an embodiment in which a plurality of amplitude addresses are set, in the step of obtaining energy information of the plurality of pulses to be measured (step S150), the energy information of the pulses to be measured may be determined according to the pulse count in the amplitude addresses and the amplitude-energy mapping relationship data provided in step S110, as described further below. In contrast, in the embodiment in which a plurality of energy addresses are set, the energy information of the pulse under test may be determined directly from the pulse count in the energy addresses (and their corresponding energy characterization values) in the step of obtaining the energy information of the plurality of pulses under test (step S150).

In a further embodiment, the specific features described above with reference to energy addresses may be applied in a non-contradictory manner to embodiments where multiple amplitude addresses are provided, where applicable. Furthermore, in the embodiments described below, such as the embodiment of step S140, described in terms of energy addresses and corresponding pulse voltage amplitudes, it will be appreciated that these embodiments may equally be implemented based on amplitude addresses, and that new embodiments thus obtained fall within the scope of the present application.

With continued reference to fig. 1, the method for obtaining a substance component may further include step S140, based on the set plurality of addresses, of determining addresses corresponding to the plurality of pulses to be measured according to a comparison result between the magnitude of the plurality of pulses to be measured and the magnitude characterization value of the plurality of addresses.

In some embodiments, the address where each pulse under test falls may be determined by means of dynamic processing. In some embodiments, the dynamic processing involves dynamic processing of the amplitude of the pulse to be measured such that there may be variations in the amplitude of the pulse that is subsequently used for comparison. In other embodiments, the dynamic processing involves setting the comparison threshold of the comparator to be dynamically changeable. In some embodiments of the present application, a combination of both is also possible.

In other embodiments, the number of dynamic threshold comparisons may also be reduced by pre-screening the address range.

In some embodiments, the address where each pulse under test falls may also be determined by way of non-dynamic processing of the gate output.

In an embodiment of dynamically processing pulses as shown in fig. 2, step S140 may include:

s210: comparing the amplitude of each pulse to be detected with comparison thresholds of a plurality of comparators in sequence;

s220: selectively adjusting the amplitude of the pulse to be measured according to the previous comparison result before comparison; and

s230: and determining the channel address corresponding to each pulse to be tested according to the comparison results of the comparators.

In the embodiment shown in fig. 2, the selective adjustment may be that if the amplitude of the pulse to be measured is smaller than the comparison threshold of the previous comparator, the amplitude of the pulse to be measured is not adjusted, and if the amplitude of the pulse to be measured is greater than or equal to the comparison threshold of the previous comparator, the amplitude of the pulse to be measured is reduced. In a specific embodiment, the reduced value of the amplitude of the pulse to be measured is the comparison threshold of the previous comparator.

In the embodiment shown in FIG. 2, the comparison thresholds of the plurality of comparators may be based on theAn amplitude characterization value for the plurality of addresses is determined. In a further embodiment, the comparison threshold of the plurality of comparators is part of the magnitude characterizing values of the plurality of addresses. In a preferred embodiment, the comparison thresholds of the plurality of comparators are each determined by sequentially bisecting the amplitude characterizing values of the plurality of sequentially determined addresses (referred to herein simply as bisected addresses). In one embodiment, the comparison threshold of the plurality of comparators may be defined by (1/2) N, (1/2) for N addresses ² ×N,·(1/2) ³ The amplitude characterization values of the x N and … … are determined until the specific address of the pulse to be detected can be determined by comparison. In one example, for example, n=256, the comparison threshold of the plurality (e.g., 8) of comparators may be determined by the magnitude characterizing values of 128, 64, 32, 16, 8, 4, 2, 1 track, e.g., V128, V64, V32, V16, V8, V4, V2, V1.

Thus, in the embodiment of the present application, the pulse is dynamically processed, so that the amplitude of the pulse input to each stage of comparator is changed.

In particular, the selective dynamic adjustment (reduction) of the amplitude of the pulse to be measured can be achieved by combining a subtractor or subtracting circuit, a gate or gating circuit and optionally a processing unit.

In the specific embodiment shown in fig. 3, step S220 may include:

s310: setting a gating device according to a previous comparison result, wherein the gating device is provided with a first gating branch and a second gating branch which are used for selectively outputting pulses to be tested;

s320: inputting the pulse to be tested into a set gating device;

s330: delay processing is carried out on the pulse to be detected output from the first gating branch; and

s340: the amplitude of the pulse to be measured output from the second gating arm is subtracted.

In an alternative embodiment, the step S310 includes: the comparison result of the previous comparator is input into the processing unit, and the gate is set by the processing unit.

A specific example of dynamic processing of pulses is described below with reference to fig. 2-4. Fig. 4 shows a first block architecture diagram for implementing dynamic processing of pulses. In this particular example, the number of energy addresses is 256, which has an amplitude characterization value denoted V1-V256.

As shown in fig. 4, the module architecture, which may also be referred to as an address determination unit 400, may include a plurality (e.g., 8) of comparators 410, a plurality (e.g., 7) of gates 420, and a processing unit 430 connecting the comparators and gates. Each of the gates 420 may include a first gate branch 421 and a second gate branch 422 for selectively outputting a pulse to be measured, wherein a delay 440 may be provided in the first gate branch 421 and a subtractor 450 may be provided in the second gate branch 422. As shown in fig. 4, the subtractor 450 may set a reduction value by the processing unit 430, and the reduction value may be a comparison threshold value of the previous comparator 410.

In the illustrated embodiment, the plurality of comparators 410 are configured as multi-stage parallel comparators, and the pulse signal under test is selectively dynamically adjusted to the amplitude of the pulse signal under test according to the comparison result of the previous stage (e.g., n-stage) comparator before being input to the next stage (e.g., n+1-stage). In the particular embodiment shown in fig. 4, selective dynamic adjustment may be achieved by a delay 440 and a subtractor 450 provided in a gate 420 and a first gate leg 421 and a second gate leg 422 thereof, respectively, provided between adjacent two stages of comparators 410.

Taking 256 total energy addresses as an example, referring to fig. 2 to fig. 4, the implementation process of the selective dynamic adjustment is specifically described as follows:

0) A threshold voltage V00 slightly greater than the maximum amplitude of the noise signal may be set to the 0 th stage comparator (not shown in fig. 4) and subsequent selective dynamic adjustment of the pulse signal may be performed to determine the address after the 0 th stage comparator is triggered.

1) The comparison threshold at the first end (e.g., the F-end) of the first stage comparator may be set according to the corresponding amplitude representation value of the 128 th track address (i.e., the track address determined by the binary energy track address 256), such as the upper limit of the amplitude interval of the energy track address, which may be represented by V128. When a pulse enters the second end (such as the P end) of the first-stage comparator, if the pulse energy is smaller than the energy sign value of the 128 th channel address, the amplitude of the pulse is correspondingly smaller than the comparison threshold value of the 128 th channel address, and the comparator outputs a result level 0; if the pulse energy is more than or equal to the energy representation value of the 128 th track address, outputting a result level 1.

2) The pulse signal will also enter the second stage comparator, more specifically the P-terminal of the second stage comparator. At this time, the address number corresponding to the second stage comparator is determined by dividing the address number corresponding to the previous stage comparator into two. Here, the F-side comparison threshold of the second-stage comparator may be set according to the amplitude representing value corresponding to the 64 th track address (i.e., the track address determined by dividing the previous track address), and the upper limit of the amplitude interval of the energy track address may be represented by V64, for example.

The pulse signal will also undergo selective dynamic adjustment before entering the second stage comparator. Here, when the first-stage comparator outputs level 0, the pulse entering the second-stage comparator coincides with the pulse entering the first stage; when the output of the first stage comparator is 1, V128 will be reduced here according to the previous comparison threshold of the pulse amplitude.

Here, the pulse passes through a gate circuit, a subtractor circuit, and a delay circuit before entering the second-stage comparator. Therefore, when the output result of the first-stage comparator is 0, the gate selects to not process the pulse amplitude, and enters the second-stage comparator after passing through the delay device, and the arrival time of the pulse entering the second-stage comparator is consistent under two output states of the gate; when the output of the first stage comparator is 1, the gate selects to pass the pulse through the subtractor circuit, reducing the pulse amplitude by V128.

3) Similarly, the pulse signal will also continue into the third stage comparator, more specifically into the P-terminal of the third stage comparator. At this time, the number of addresses corresponding to the third-stage comparator is determined by dividing the number of addresses corresponding to the previous-stage comparator into two. Here, the F-side comparison threshold of the third stage comparator may be set according to the amplitude representing value corresponding to the 32 nd track address (i.e., the track address determined by dividing the previous track address), and the lower limit of the amplitude interval of the energy track address may be represented by V32, for example.

The pulse signal is also subjected to selective dynamic adjustment before entering the third stage comparator. When the output level of the second-stage comparator is 0, the pulse entering the third-stage comparator is consistent with the pulse entering the second stage after being processed by the delay device; when the output result of the second-stage comparator is 1, the previous pulse amplitude is compared with a threshold value after being processed by a subtracter, and V64 is reduced.

4) The pulse amplitude to be measured can be selectively dynamically adjusted accordingly with reference to steps 2) and 3). In the case of a total energy address of 256, the comparison threshold values of the fourth to eighth comparators can be set by the corresponding amplitude characterizing values of the 16 th, 8 th, 4 th, 2 nd and 1 st addresses, respectively, and the upper limit of the amplitude interval of the energy address can be represented by V16, V8, V4, V2 and V1.

5) And counting the output result of each stage of comparator to determine the address of the channel in which the pulse to be tested falls. For example, when the output of the 8-stage comparator is binary 00000000, the pulse energy is 1 st track, from 00000000, each 1-stage increment is increased by one-stage energy track, when the output of the 8-stage comparator is binary 10000000, the pulse energy is 129 th track address, and when the output of the 8-stage comparator is binary 11111111, the pulse energy is 256 th track address.

With continued reference to fig. 5 and 6, another embodiment in accordance with the present application is shown. In the embodiments shown in fig. 5 and 6, the address where each pulse under test falls can be determined by means of non-dynamic processing of the gate output.

In the embodiment shown in fig. 5, step S140 may include:

s510: inputting each pulse to be tested into a multi-stage gate array so that the pulse to be tested sequentially passes through each stage gate of the multi-stage gate array;

s520: before the pulse to be tested passes through each stage of gate, comparing the pulse to be tested with a comparator associated with the passed gate, setting the gate according to the comparison result, and determining a gate branch of the gate outputting the pulse to be tested; and

s530: and determining the channel address corresponding to the pulse to be detected according to the output of the multi-stage gate array.

In the embodiments of the present application as shown in fig. 5 and 6, a specific example of determining the address of the channel where each pulse under test falls according to the non-dynamic processing manner of the gate output is provided. Fig. 6 shows a second block diagram for determining the address of the track in which the pulse under test falls. In this particular example, the number of energy addresses may likewise be 256, which has an amplitude characterization value denoted V1-V256.

As shown in fig. 6, the module architecture, which may also be referred to as an address determination unit 600, may include a multi-stage array of gates with each gate 611, 612', 613, … …, 618 having an associated comparator 621. For simplicity, fig. 6 shows only the comparator 621 associated with the first stage gate 611. Furthermore, although not shown in fig. 6, it is contemplated that the module architecture may also include a processing unit.

As shown in fig. 6, each of the gates 611, 612', 613, … …, 618 may have a first gate arm 6111 and a second gate arm 6112 for selectively outputting a pulse to be measured, the gate of the non-final stage is connected to the two gates of the next stage through the first and second gate arms, respectively, and the first and second gate arms 6181, 6182 of the gate of the final stage may serve as the output of the multi-stage gate array.

In embodiments of the present application, a multi-stage gate array may be constructed based on dichotomy. In a further embodiment, the first stage gate corresponds to a first address determined by a total address number of the plurality of addresses and two address intervals for the lower stage gates are defined by the first address; the other gates correspond to a second address determined by dividing the address interval defined by the upper gate to which they are connected into two, and two address intervals for the lower gate or for output are defined by the second address. Accordingly, the comparison threshold of each comparator is determined by the amplitude characterization value of the corresponding address of the associated gate.

In the specific example shown in fig. 6, the corresponding address of the first stage gate 611 may be determined by halving the total energy address, e.g., the 128 th address, and accordingly define two address intervals for the lower stage gates 612, 612', e.g., the 1 st to 128 th addresses, i.e., [1,128] and the 129 th to 256 th addresses, i.e., [129,256]. Accordingly, the comparison threshold of the comparator 621 associated with the first stage gate 611 may be determined based on the magnitude characterization value of the 128 th track address, such as V128.

Further, in the embodiment shown in fig. 6, the two address intervals may be allocated accordingly according to the strobe branches to which the lower-stage strobes are connected. As shown in fig. 6, the second stage gate 612 of the first gate branch 6111 connected to the first stage gate 611 may allocate a track address interval from the 1 st track address to the 128 th track address, and accordingly corresponds to a track address, such as a 64-track address, corresponding to the two-division of the track address interval. As shown in fig. 6, the second stage gate 612' of the second gate branch 6112 connected to the first stage gate 611 may allocate a track address interval from the 129 th track address to the 256 th track address, and accordingly corresponds to a track address, such as 192 track addresses, corresponding to the two branches of the track address interval. Accordingly, the comparison threshold of the comparator (not shown) associated with the second stage gate 612 may be determined based on the magnitude characterization value of the 64 th track address, such as V64; the comparison threshold of the comparator (not shown) associated with the second stage gate 612' may be determined based on the amplitude characterization value of the 192 th address, such as V192.

The address corresponding to the gate of the subsequent stage and the comparison threshold of the associated comparator can be determined accordingly.

Thus, it will be appreciated that the two gating branches of the last stage (e.g., stage 8) gate may constitute the output of the multi-stage gate, and that the address where the pulse under test falls may be determined from the output of the multi-stage gate. For example, as shown in fig. 6, when a pulse under test is output by the first strobe branch 6181 of the 8 th stage strobe 618, this means that the pulse under test falls within the 1 st address.

It will be appreciated that the method features or module architecture features described in relation to other embodiments may be combined with the embodiments shown in fig. 5 and 6 in a non-contradictory manner, as desired.

In further embodiments, pulses, such as the address of the track that a blinking pulse falls into, may be counted by setting a dynamic comparison threshold, as previously described.

In further embodiments, setting the dynamic comparison threshold may be achieved by a multi-level comparison or a single-level comparison.

In the embodiment shown in fig. 7, the dynamic comparison threshold is shown set by a multi-level comparison. Specifically, step S140 may include:

s710: making the amplitude of each pulse to be measured perform first-stage comparison of multi-stage comparison to determine the address interval in which the pulse to be measured falls, wherein each stage comparison defines at least two address intervals through at least one comparison threshold;

S720: sequentially carrying out next-stage comparison to determine the address interval in which the pulse to be detected falls until the final-stage comparison is completed, wherein the comparison threshold value of the next-stage comparison is determined according to the address interval determined by the previous-stage comparison; and

s730: and determining the address of the channel where the pulse to be detected falls according to the comparison result of the last stage.

In the embodiment of the application, by endowing the comparator with the dynamically changing threshold value, the scintillation pulse can be counted according to the energy address.

By way of illustration and not limitation, the above-described multi-level comparison may be implemented by different types of multi-level comparison units, which may be or include the track address determination unit. It is contemplated that the modular architecture of the multi-level comparison unit may or may not have an "entity" multi-level comparison structure, so long as a dynamic threshold-based multi-level comparison can be achieved, and that embodiments of the present application are intended to cover both cases.

For example, in some embodiments, a multi-level comparison without a "physical" multi-level comparison structure may be implemented by a single or multiple comparators connected to multiple parallel delay lines, where multiple different comparisons in a peer or different levels of comparison may be implemented by different delays of the delay lines in combination with adjustable comparators.

For example, in further embodiments, a "physical" multi-level comparison structure may be provided that corresponds to a multi-level comparison, the number of levels of the "physical" multi-level comparison structure corresponding to the number of levels of the multi-level comparison, the number of comparators in each level comparison structure corresponding to the number in each level comparison.

An exemplary module architecture of the above-described embodiments will be described below with reference to the accompanying drawings.

In some preferred embodiments, the number of comparison thresholds for each level of comparison is the same, such that the number of address intervals defined by the comparison thresholds for each level of comparison is the same.

In a further preferred embodiment, the comparison threshold of each level comparison defines an address interval that is equally divided. Here, in one embodiment, the comparison threshold set by the first level comparison is such that the comparison threshold of the first level comparison defines an address interval that bisects the plurality of addresses; the comparison threshold value set by the next-stage comparison is such that the address interval defined by the comparison threshold value of the next-stage comparison is equally divided into the address intervals determined by the previous-stage comparison.

Specifically, the total energy address number is n=m ⁿ (e.g., n=256), the pulse to be detected may be subjected to (m-1) ×n (m is equal to or greater than 2) threshold comparisons by setting a dynamic threshold to determine the m in which the pulse falls ⁿ An energy address in the addresses, where n is the number of stages and m is the number of pulse (maximum) amplitude intervals for each stage defined by a predetermined (m-1) comparison threshold. It will be appreciated that in view of the correspondence of energy addresses, energy intervals and pulse amplitude intervals, embodiments of the present application contemplate dividing m amplitude intervals, energy intervals and/or equivalent substitutions of address intervals.

As previously mentioned, the modular architecture of the multi-stage comparison unit may not have a "physical" multi-stage comparison structure, such as implemented by different delays of the delay line in combination with a tunable comparator.

In this embodiment, the multi-level comparison is performed by a first multi-level comparison unit that does not have a physical multi-level comparison structure. The first multi-stage comparison unit may include a plurality of parallel delay lines connected to the pulse input to be measured, an adjustable comparator connected to the delay lines, and an arbiter operatively connected to the adjustable comparator, wherein delay times of at least some of the delay lines are different.

In a further embodiment, the adjustable comparator is a single one, and the delay times of the plurality of parallel delay lines are different.

In a further embodiment, the total energy addresses are n=m ⁿ For example, n=256, and the maximum (m-1) ×n (m is greater than or equal to 2) threshold comparison is performed on the scintillation pulse to be tested, which can be implemented by using only (m-1) ×n parallel delay lines in combination with a single comparator.

The embodiments shown in fig. 8 and 10 implement the energy address division of the pulse signal by using only one comparator in combination with a delay line, where the threshold value set at the negative input of the comparator is determined by the arbiter. By providing corresponding delay lines, different comparison thresholds can be set when pulse signals with different delays are received. Specifically, when the pulse signal is externally input into the first multi-stage comparing unit, the pulse signal is respectively fed into a plurality of lines with unequal delays, and the plurality of loops finally input the signal to the positive input end of the same comparator, namely, the pulse is respectively input into the comparator at a plurality of time points at a certain time interval.

The embodiment of the application covers different setting modes of the comparator threshold values and corresponding matching modes of the delay lines.

In the embodiment shown in fig. 8, the comparison threshold for each level of comparison is 1, so that two halves define two address intervals, i.e. m=2.

As shown in fig. 8, the total energy address number is n=m ⁿ For example (e.g., n=256) (fig. 9), the first multi-stage comparison unit 800 includes a plurality (8) of delay lines 8101-8108 with unequal delays, an adjustable comparator 820 coupled to the delay lines 8101-8108, and an arbiter 830 operatively coupled to the adjustable comparator 820.

The comparison process is described below in conjunction with fig. 8 and 9.

When a pulse signal is input to the first-stage comparing unit 800, the pulse signal is respectively fed to a plurality of (8) delay lines 8101-8108 with unequal delays, and the plurality of (8) delay lines 8101-8108 are input to the positive input end of the same adjustable comparator 820, that is, the pulse is respectively input to the comparator at eight time points at certain time intervals.

The threshold value set at the negative input end of the adjustable comparator 820 is determined by the arbiter 830, and the arbiter can set the comparison threshold value of the adjustable comparator 820 according to the set amplitude representing value of the channel address, so as to realize that the pulse amplitudes corresponding to different pulse energies are sequentially input to the negative input end of the comparator to be compared with the pulse to be tested.

A dichotomy multistage comparison example is schematically shown in fig. 9. If the total energy address number is N=m ⁿ (e.g., n=256), i.e., 2 ⁸ The addresses will be compared (2-1) x 8=8 times. The unequal delays are schematically shown in fig. 8 as a number of different delays, i.e. after 8 different delays (achieving the effect of inputting one signal cycle eight times). In the embodiment shown in fig. 8 and 9, 8-level comparisons will be implemented and the comparison threshold for each level comparison is 1, but there is no physical 8-level comparison structure, but only 1 adjustable comparator is utilized.

With continued reference to FIG. 9, first, two address intervals, i.e., 1 st to 128 th addresses and 129 th to 256 th addresses (which may also be represented by amplitude intervals, such as V1-V128 and V129-V256), are obtained in a first level comparison based on the total energy address number in two, the corresponding comparison threshold being an amplitude indicative of the 128 th address, such as V128.

If the pulse signal amplitude can cross the comparison threshold V128 through the first-stage comparison, the first-stage comparison result is that the pulse amplitude is in V129-V256, and the second-stage comparison threshold is determined based on the address interval (amplitude interval) in which the pulse signal determined by the first-stage comparison falls, for example, the second-stage comparison threshold may be set as V192, so that two address intervals (amplitude intervals) of the second stage are further defined by two boundaries, for example, V129-V192, V193 to V256.

After the second-stage comparison, if the pulse signal amplitude can cross the comparison threshold V192, the second-stage comparison result is that the amplitude is between V193-V256. Accordingly, the comparison threshold for the third stage may be determined based on the address interval (amplitude interval) determined by the second stage comparison, and may be set to V224, for example, to further two-way delimit the two address intervals (amplitude intervals) for the third stage, such as V193-V224, V225 to V256.

And through third-stage comparison, if the amplitude of the pulse signal can exceed the comparison threshold V224, the amplitude is between V225 and V256 as a result of the third-stage comparison. Accordingly, the comparison threshold for the fourth stage may be determined based on the address interval (amplitude interval) determined by the third stage comparison, and may be set to V240, for example, to further two-way delimit the two address intervals (amplitude intervals) of the fourth stage, such as V225-V240, V241 to V256.

After the fourth comparison, if the pulse signal amplitude can cross the threshold V240, the fourth comparison result is that the amplitude is between V241-V256. Accordingly, the comparison threshold of the fifth stage may be determined correspondingly based on the address interval (amplitude interval) determined by the fourth stage comparison, and may be set to V248, for example, to further two-boundary the two address intervals (amplitude intervals) of the fifth stage, such as V241-V248, V249 to V256.

And through fifth-stage comparison, if the amplitude of the pulse signal can exceed the threshold value V248, the amplitude of the fifth-stage comparison result is between V249-V256. Accordingly, the comparison threshold value of the sixth level may be determined correspondingly based on the address interval (amplitude interval) determined by the fifth level comparison, and may be set to V252, for example, so as to further two-delimit two address intervals (amplitude intervals) of the sixth level, such as V249-V252, V253 to V256.

After the sixth comparison, if the pulse signal amplitude can cross the threshold V252, the sixth comparison result is that the amplitude is between V253-V256. Accordingly, the comparison threshold of the seventh level may be determined correspondingly based on the address interval (amplitude interval) determined by the sixth level comparison, e.g. may be set to V254, thereby further two demarcating the two address intervals (amplitude intervals) of the seventh level, e.g. V253-V254, V255 to V256.

Through the seventh comparison, if the pulse signal amplitude can cross the threshold V254, the seventh comparison result is that the amplitude is between V255-V256. Accordingly, the comparison threshold value of the eighth stage can be correspondingly determined on the basis of the address interval (amplitude interval) determined by the seventh stage comparison, and can be set to V255, for example, so that two address intervals (amplitude intervals), here two addresses (amplitudes), such as V255, V256, of the eighth stage are further defined by the two boundaries. The pulse signal amplitude can cross the comparison threshold V255, then the pulse signal amplitude is between V255 (excluding) -V256, then the pulse signal is at the 256 th energy address. It can be seen that the energy address corresponding to the pulse (amplitude) can be determined by 8 comparisons.

Here, when the pulses on all delay lines pass through the comparator, it can be determined which address the pulse corresponds to according to the output result of the comparator.

In the embodiment of the application, the arbiter may be implemented by a Micro Control Unit (MCU), and the arbiter may control the change of the comparison threshold value by a digital-to-analog converter (DAC).

As previously described, the conventional MVT method employs fixed threshold and complex fitting calculations, is limited to specific energy segments, requires precise time information, and has dead time. This results in disadvantages of low processing efficiency, large consumption of hardware resources, poor high temperature tolerance, and the like. In contrast, the present embodiment directly samples and classifies unknown pulses to corresponding energy addresses through dynamic threshold settings and simplified processing. In this way, fitting calculations, TDC and accurate time information are not required. Compared with the traditional method, the pulse energy acquisition process is simplified, hardware resources are saved, the power consumption of the FPGA is reduced, and the high-temperature tolerance capability is improved. In addition, the dead time is greatly shortened through threshold comparison and table lookup operation, continuous pulse processing can be realized, and the system performance is effectively improved.

It is contemplated that in other embodiments, the comparison threshold may be greater than 1 for each level of comparison.

In the embodiment shown in fig. 10, the comparison threshold for each stage is 3, so that four address intervals are defined by four, i.e., m=4. Also, the total energy address number is N=m ⁿ For example (e.g., n=256), the multi-level comparison is 4 levels, each with 3 comparison thresholds.

Similar to the embodiment shown in fig. 8, in the embodiment shown in fig. 10, only one comparator is used in combination with a delay line to achieve the energy address division of the pulse signal, where the threshold value set at the negative input of the comparator is determined by the arbiter.

As shown in fig. 10, the first multi-stage comparing unit 1000 includes a plurality of (12) delay lines 10101-10112 with unequal delays, an adjustable comparator 1020 connected to the delay lines 10101-10112, and an arbiter 1030 operatively connected to the adjustable comparator 1020.

The comparison process is described below in conjunction with fig. 10 and 11.

As previously described, in the embodiment shown in fig. 10, the module architecture of the first multi-stage comparison unit 1000 may not have a "physical" multi-stage comparison structure, but rather implement multi-stage comparison through multiple parallel delay lines and a single adjustable comparator.

In the specific embodiment shown in fig. 10, after the first-stage comparison, the address interval determined by the first-stage comparison is subjected to quarter division, the arbiter sequentially sets a corresponding comparison threshold for the second-stage comparison, and according to the second-stage comparison result, the address interval determined by the second-stage comparison is further subjected to quarter division, thereby sequentially completing all the multi-stage comparisons.

Thus, depending on the address interval in which the pulse falls, if each stage only needs to compare the comparison threshold once to determine the address interval in which the pulse falls, the energy address can be determined at least 4 times; if each stage needs to compare 3 comparison thresholds to determine the falling address interval, the energy address can be determined up to 12 times. Accordingly, due to the absence of a "physical" multi-stage comparison structure, the aforementioned plurality (12) of delay lines 10101-10112 with unequal delays may be dynamically adapted to different comparison times of the multi-stage comparison, such as between 4 and 12 times. In the embodiment shown in fig. 10, the comparison threshold for comparison is preferably from small to large at peer comparison.

One specific example of a quarter bounding four address intervals is described with continued reference to fig. 10 and 11.

In the first level comparison, the arbiter 1030 may set 3 comparison thresholds, such as V64, V128, V192, for the first level comparison. Preferably, in the first level comparison, V64, V128, V192 are compared in order from small to large, and after determining the address interval in which the pulse falls, the remaining comparison threshold may not be compared any more. For example, in the example shown in FIG. 11, the pulse is at track 193, and its corresponding amplitude characterization value is denoted, for example, as V193. Thus, the pulse amplitude sequentially crosses the 1 st comparison threshold V64, the 2 nd comparison threshold V128, and the 3 rd comparison threshold V192 of the first-stage comparison. From this, it can be determined that the amplitude range in which the pulse is located is V193-V256, i.e., within the 193 th to 256 th track address interval.

In the second level comparison, the arbiter 1030 may determine which of V1 (0) -V64, V65-V128, V129-V192, or V193-V256 (e.g., V193-V256 described above) the address interval (amplitude interval) is located according to the first level comparison result, and set 3 comparison thresholds for the second level comparison in the address interval determined by the first level comparison accordingly to quarter the address interval determined by the first level comparison, thereby completing all four level comparisons in turn.

For example, assume that the pulse amplitude is at addresses 1-64, specifically 1-4 (not shown), namely 0-V64 (specifically V4):

setting a 1 st comparison threshold value (minimum threshold value) V64 of the first stage to the comparator, if the first pulse signal entering the comparator is compared with the threshold value, if the threshold value cannot be crossed, the amplitude of the pulse signal is between 0 and V64;

further, a comparison threshold value of the second stage is set for the threshold value of the comparator, then a 1 st comparison threshold value (minimum threshold value) V16 which is set for the comparator as the second stage is selected, a delayed second pulse signal is input into the comparator, and if the threshold value V16 cannot be crossed, the amplitude of the pulse signal is between 0 and V16;

Further, a comparison threshold value of a third level is set for the threshold value of the comparator, then a 1 st comparison threshold value (minimum threshold value) V4 which is set for the comparator as the third level is selected, a delayed third pulse signal is input into the comparator, and if the threshold value V4 cannot be crossed, the amplitude of the pulse signal is between 0 and V4;

further, a comparison threshold value of a fourth stage is set for the threshold value of the comparator, then a 1 st comparison threshold value (minimum threshold value) V1 which is set for the comparator as the fourth stage is selected, a delayed pulse signal is input into the comparator, and if the threshold value V1 cannot be crossed, the amplitude of the pulse signal is between 0 and V1, namely the 1 st energy address is located; if the pulse signal crosses V1, the comparator is provided with a 2 nd comparison threshold V2 of the fourth stage, and if the pulse signal cannot cross the threshold V2, the amplitude of the pulse signal is between V1 and V2, namely the energy address 2; if the pulse signal crosses V2, the comparator is provided with a 3 rd comparison threshold V3 of a fourth stage, and if the pulse signal cannot cross the threshold V3, the amplitude of the pulse signal is between V2 and V3, namely the 3 rd energy track address; if the pulse signal crosses V3, the amplitude of the pulse signal is between V3-V4, i.e., at the 4 th energy track.

Thus, the embodiment of FIG. 10 in which the comparison threshold is determined using the quartile method has the advantage of the simple embodiment of FIG. 8 in which the comparison threshold is determined using the dichotomy method. In addition, the embodiment shown in fig. 10 realizes the dynamic threshold spectrum formation of bit expansion by adopting the quartering method, thereby having better working efficiency and structural flexibility, and the comparator chain (i.e. the number of comparators and the comparison level number of each stage) can be adjusted according to different requirements of application scenes.

Unlike the embodiment shown in fig. 10, the embodiment shown in fig. 12 employs a plurality of comparators in combination with delay lines to achieve energy addressee division of the pulse signal.

Thus, in the embodiment shown in fig. 12, there are a plurality of adjustable comparators, different comparators are connected to different delay lines, and delay times of delay lines connected to the same comparator are different.

As shown in fig. 12, the first multi-stage comparing unit 1200 includes a plurality (12) of delay lines 12101-12112 with unequal delays, a plurality (3) of adjustable comparators 1221-1223, and an arbiter 1230 operatively coupled to the adjustable comparators 1221-1223. The plurality (12) of delay lines 12101-12112 having unequal delays are divided into a plurality of sets of delay lines corresponding to the plurality (3) of adjustable comparators 1221-1223, each set being connected to one of the adjustable comparators. The delay times of the same group of delay lines, such as 12101-12104, 12105-12108 or 12109-12112, connected to the same adjustable comparator are different. But as shown in fig. 12, the sets of delay lines may have the same delay configuration.

Here, the first multi-level comparison unit 1200 shown in fig. 12 may be used to implement multi-level comparison based on the dynamic comparison threshold, which is not described herein.

In a preferred embodiment, the number of the plurality of adjustable comparators may correspond to a comparison threshold number of each stage of comparison. For example, in the embodiment shown in fig. 12, the number of adjustable comparators (3) corresponds to the number of comparison thresholds per stage based on the quartering method. In this preferred embodiment, a comparison of different comparison thresholds of peers may be achieved simultaneously.

As previously described, a "physical" multi-level comparison structure corresponding to the multi-level comparison may also be provided to impart a dynamically varying threshold to the comparator, enabling the scintillation pulses to be counted in terms of energy addresses.

An exemplary module architecture for an embodiment having a "physical" multi-level comparison structure will be described below in conjunction with the accompanying drawings. In this embodiment, the multi-stage comparison is performed by a second multi-stage comparison unit having a physical multi-stage comparison structure. The second multi-stage comparison unit comprises a plurality of comparator subunits connected with pulse input to be detected and an arbiter operatively connected with the plurality of comparator subunits, wherein each comparator subunit corresponds to one of the multi-stage comparison units and comprises a single or a plurality of parallel adjustable comparators, and a delay device is arranged between adjacent comparator subunits.

In a further embodiment, the total energy addresses are n=m ⁿ For example, n=256, and the comparison of the (m-1) x N (m is greater than or equal to 2) sub-threshold values is performed on the scintillation pulse to be tested at most, and the comparison can be implemented by adopting N stages of comparator subunits (each stage of comparator subunits has (m-1) comparators) and combining a delay between adjacent stages of comparator subunits.

In the embodiment shown in fig. 13, a physical multi-stage comparator subunit (8 stages) is provided, with 1 physical comparator per stage, so that two branches define two address intervals, i.e., m=2.

In terms of multi-level comparison, the embodiment shown in fig. 13 is similar to the embodiment shown in fig. 8. Referring to fig. 13 and 9 in combination, if the total energy address number is n=m ⁿ (e.g., n=256), i.e., 2 ⁸ The addresses will be compared (2-1) x 8=8 times.

Thus, as shown in fig. 13, the second multi-stage comparison unit 1300 includes a plurality of (8) comparator subunits 1310 connected to the pulse input under test and an arbiter 1320 operatively connected to the plurality of comparator subunits 1310, wherein each comparator subunit 1310 corresponds to one of the plurality (8) stage comparisons and includes a single adjustable comparator 1311, with a delay 1330 disposed between adjacent comparator subunits.

With continued reference to fig. 13 and 9, each stage may employ a comparator to compare with the peak pulse voltage, and each comparison may determine between two address intervals (amplitude intervals), i.e., above or below the comparison threshold set by the stage comparator, and after 8 stages of comparison, it may be determined which of the 256 addresses the pulse falls into, thereby forming, for example, 256 energy spectra. In the example shown in fig. 13, a threshold voltage may be input to the negative input terminals of the adjustable comparators of each stage of the comparator subunits, and a delay device may be provided between each stage of the comparator subunits to form a slight delay (for example, 5 ns), for example, whereby pulse signals serially input to the positive input terminals of the comparators of the plurality of (8) comparator subunits are respectively processed by the plurality of (8) comparator subunits at different delay times, and it is possible to determine which energy address the pulse, for example, the scintillation pulse, is located after passing through the final stage, for example, the 8 th stage of the comparator.

A specific example of determining in which energy track address the pulse amplitude of an input pulse, such as a scintillation pulse signal, is located in the pulse amplitude section corresponding to using the second multi-stage comparison unit 1300 shown in fig. 13 based on the dichotomy will be described below with reference to fig. 9.

According to the dichotomy, the middle energy address of the 1-256 energy addresses is the 128 th energy address, a first comparison threshold, namely, the amplitude representing value of the 128 th energy address, can be set for the comparator of the first-stage comparator subunit according to the middle energy address, and two address intervals, namely, the 1-128 energy addresses and the 129-256 energy addresses, can be defined by the comparison threshold. And comparing the amplitude of the input pulse signal with a first comparison threshold value to judge whether the pulse signal is positioned in a 1-128 energy address interval or a pulse peak value interval corresponding to 129-256 energy addresses. If the comparator output is 1, which indicates that the pulse peak value of the input signal has crossed the pulse amplitude representing value corresponding to the 128 th energy address, the input pulse signal is located in the 129 th to 256 th address interval; if the comparator output is 0, the peak value of the input pulse signal is located in the 1 st to 128 th address interval if the peak value of the input pulse signal does not exceed the pulse amplitude representing value corresponding to the 128 th energy address. The comparison result of the comparator of the first-stage comparator subunit is input into the arbiter, the arbiter judges which energy address interval or the pulse amplitude interval corresponding to the energy address interval the input pulse signal is positioned in according to the comparison result, and the comparison threshold value is continuously set for the comparator of the second-stage comparator subunit by a dichotomy according to the energy address interval, and the like until the comparator of the last-stage comparator subunit determines which energy address the input scintillation pulse signal is positioned in, and then, for example, the pulse count in the energy address can be increased by 1 by the counting unit. For example, for a 256-track energy address, the 1 st track address may correspond to 00000000 and the 256 th track address may correspond to 11111111.

It will be appreciated that if a more accurate energy spectrum is desired, the length of the comparator chain, i.e. the number of comparators per stage and the number of comparator stages, can be increased.

In the embodiment shown in fig. 14, a physical multi-stage comparator subunit (4 stages) is provided, with 3 physical comparators per stage, so that four address intervals are defined by four, i.e., m=4.

In terms of multi-level comparison, the embodiment shown in fig. 14 is similar to the embodiment shown in fig. 10. Referring to fig. 14 and 11 in combination, if the total energy address number is n=m ⁿ (e.g., n=256), i.e., 2 ⁸ The addresses will be compared 4 times.

Thus, as shown in fig. 14, the second multi-stage comparing unit 1400 includes a plurality of (4) comparator subunits 1410 connected to the pulse input to be measured and an arbiter 1420 operatively connected to the plurality of comparator subunits 1410, wherein each comparator subunit 1410 corresponds to one of the plurality of (4) stage comparisons and includes a plurality of (3) parallel adjustable comparators 1411-1413, with a delay 1430 disposed between adjacent comparator subunits.

It will be appreciated that the features of the embodiments of fig. 10 and 13 may be incorporated into the embodiment of fig. 14 in a non-contradictory manner as required to arrive at a new embodiment, and are not described in detail herein.

A specific example of determining in which energy track address the pulse amplitude of an input pulse, such as a scintillation pulse signal, is located in the pulse amplitude section corresponding to using the second multi-stage comparison unit 1400 shown in fig. 14 based on the quartering method will be described below in conjunction with fig. 11.

In the specific example shown in fig. 14, a physical 4-stage comparator subunit 1410 is provided, each with 3 physical adjustable comparators, whereby 4 address intervals (or 4 energy intervals or amplitude intervals) can be defined. Here, it can be expressed as n=4, m=4, i.e. there are n=4-level comparisons, each level dividing the unknown energy range into m=4 energy intervals.

Referring to fig. 14 and 11 in combination, the negative inputs of the 3 comparators of the first stage comparator subunit may determine the 3 comparison thresholds of the first stage, e.g., denoted as V64, V128, V192, based on the 64 th, 128 th, 192 th track address of the quarter 256 track address. If the pulse amplitude (peak value) to be measured only passes V64 and not V128, the arbiter can determine that the energy of the pulse is between lanes 64 and 128. Therefore, in the second-stage comparison, the arbiter sets the threshold value of 3 comparators of the second-stage comparator subunit through the address interval determined by the comparison result of the previous stage, such as V65-V128, and divides the interval [ V65, V128] into four equal parts, and so on, completes four-stage comparison, and finally determines the specific address of the pulse on the energy spectrum.

Thus, the embodiment of FIG. 14 in which the comparison threshold is determined using the quartile method has the advantage of the simple embodiment of FIG. 13 in which the comparison threshold is determined using the dichotomy method. In addition, the embodiment shown in fig. 14 realizes the dynamic threshold spectrum formation of bit expansion by adopting the quartering method, thereby having better working efficiency and structural flexibility, and the comparator chain (i.e. the number of comparators and the comparison level of each stage) can be adjusted according to different requirements of application scenes.

In the embodiment shown in fig. 8-14, the comparison threshold for the first level comparison is determined based on the total number of the plurality of addresses. However, it is conceivable to determine the comparison threshold of the first-stage comparison based on pulse characteristics or other characteristics to reduce the number of comparisons.

In one embodiment, the comparison threshold for the first level comparison may be determined from a given a priori address interval. It will be appreciated that the a priori address intervals may cover corresponding energy intervals, amplitude intervals, etc.

In some embodiments, the given a priori address interval is 1, the comparison threshold of the first level comparison is 1 and is determined from an amplitude characterization value of one of the end addresses of the a priori address interval.

In one example, the total energy track number is still n=m ⁿ (e.g., n=256), for example, a first-order is determined based on pulse characteristicsThe test address interval is smaller than a certain address, such as smaller than 64 addresses, and the comparison threshold of the first stage can be determined according to the prior interval. More specifically, the comparison threshold may be determined based on the endpoint (upper) address (e.g., 64 addresses) of the a priori address interval, e.g., based on the magnitude characteristic corresponding to the 64 th address, e.g., denoted as V64. It will be appreciated that the a priori address intervals may be set according to different pulse characteristics. For example, in pulsed neutron saturation logging, considering that the address corresponding to about 80% of the pulse energy of the scintillation pulse corresponding to the gamma ray is below 64, the address interval is set to less than 64 addresses, and the comparison threshold of the first comparison is set to V64 as previously described.

In the embodiment of the present application, in the first-stage comparison, it may be determined whether the pulse is located in the a priori address interval (in the low energy section) or not located in the a priori address interval (in the high energy section). The comparison threshold may then be dynamically set in a subsequent level comparison by the principle of dichotomy or quartering.

Embodiments of determining the comparison threshold for the first level comparison from a given a priori address interval may be implemented in a multi-level comparison unit according to embodiments of the present application, i.e. based on a modular architecture of delay line combined comparators, or based on a "physical" multi-level comparator subunit architecture, such as those shown in fig. 8, 10, 12, 13, 14, or the like.

An embodiment of determining the comparison threshold for the first level comparison from a given a priori address interval, in which case the non-first level comparison is implemented by dichotomy, will be described below with reference to the second multi-level comparison unit 1500 shown in fig. 15. The second multi-stage comparing unit 1500 shown in fig. 15 is similar to the second multi-stage comparing unit 1300 shown in fig. 13, except that the second multi-stage comparing unit 1500 shown in fig. 15 has more two stages of comparator subunits, namely, ten stages of comparator subunits 1510 in total.

Furthermore, this embodiment differs from the embodiments described above in connection with fig. 13 and 9 in that the comparison threshold of the comparator 1511 in the first stage comparator subunit 1510, for example V64, is set in accordance with the upper end of the a priori address interval described above (64 th address).

If the comparison result of the first-stage comparison is that the pulse energy is in the prior address interval (in the low energy section) and the pulse amplitude is 0-V64, the comparison threshold of the comparator in the second-stage comparator subunit can be set as V32 according to the dichotomy; assuming that the pulse signal amplitude can cross the threshold V32, the pulse signal amplitude is between V32-V64, the comparison threshold of the comparator in the third stage comparator subunit can be set to V48 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V48, the pulse signal amplitude is between V32-V48, the comparison threshold of the comparator in the fourth stage comparator subunit may be set to V40 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V40, the pulse signal amplitude is between V32-V40, the comparison threshold of the comparator in the fifth-stage comparator subunit may be set to V36 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V36, the pulse signal amplitude is between V32-V36, the comparison threshold of the comparator in the sixth comparator subunit may be set to V34 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V34, the pulse signal amplitude is between V32-V34, the comparison threshold of the comparator in the seventh stage comparator subunit may be set to V33 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V33, the pulse signal amplitude is between V32-V33, i.e. the 33 th energy address. It can be seen that the energy address corresponding to the pulse amplitude is determined by 7-level comparison.

In the example where the pulse energy of the scintillation pulse is about 80% and the address is lower than 64, the 80% pulse comparison count is reduced by 1.

If the comparison result of the first-stage comparison is that the pulse energy belongs to a high-energy section (i.e. outside the prior address interval), and the pulse amplitude is positioned in V64-V256, the comparison threshold of the comparator in the second-stage comparator subunit can be set as V160 according to a dichotomy; assuming that the pulse signal amplitude can cross the threshold V160, the pulse signal amplitude is between V160-V256, the comparison threshold of the comparator in the third stage comparator subunit may be set to V208 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V208, the pulse signal amplitude is between V160-V208, the comparison threshold of the comparator in the fourth stage comparator subunit may be set to V184 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V184, the pulse signal amplitude is between V160-V184, the comparison threshold of the comparator in the fifth stage comparator subunit may be set to V172 in a dichotomy; assuming that the pulse signal amplitude can cross the threshold V172, the pulse signal amplitude is between V172-V184, the comparison threshold of the comparator in the sixth comparator subunit may be set to V178 in a dichotomy; assuming that the pulse signal amplitude cannot cross the threshold V178, the pulse signal amplitude is between V172-V178, the comparison threshold of the comparator in the seventh stage comparator subunit may be set to V175 in a dichotomy; assuming that the pulse signal amplitude can cross the threshold V175, the pulse signal amplitude is between V175-V178, the comparison threshold of the comparator in the eighth stage comparator subunit may be set to V177 in a dichotomy; assuming that the pulse signal amplitude can cross the threshold value V177, the pulse signal amplitude is between V177 and V178 and is positioned at the 178 th energy track address; if the pulse signal cannot cross the threshold V177, the amplitude of the pulse signal is between V175-V177, and the comparison threshold of the comparator in the ninth comparator subunit can be set to V176 in a dichotomy, and if the pulse signal amplitude can cross the threshold V176, the amplitude of the pulse signal is between V176-V177 and is located at the 177 th energy track. It can be seen that the energy addresses corresponding to the pulse amplitudes are determined by 8-10 level comparison.

In the example where the pulse energy of the scintillation pulses is about 80% and the address is lower than 64, since only about 20% of the pulses are located in the high energy section (i.e. outside the a priori address interval), the number of scintillation pulses is 1-2 more, but the effect of significantly reduced comparison can still be obtained for all the pulses to be measured.

The negative input of the comparator of each comparator subunit is thus based on the output of the comparator subunit of the preceding stage, the energy range divided by the arbiter is based on the principle of dichotomy to select the threshold voltage to be set at the negative input of the comparator of the next stage, and a delay is provided between the comparator subunits of each stage to form a slight delay (e.g. 5 ns), whereby the pulse signals serially input to the positive inputs of the comparators of the comparator subunits are processed by the comparator subunits respectively with different delay times, and by the last stage (determined by the arbiter based on the output of the first stage comparator) the comparator can determine at which energy address the pulse, e.g. the blinking pulse, is located.

It is conceivable that the multi-level comparison of the above embodiment may be achieved by adapting the first multi-level comparison unit shown in fig. 8, for example by adding two delay lines.

Furthermore, in embodiments where the comparison threshold for the first level comparison is determined from a given a priori address interval, the non-first level comparison may be implemented by a quartering method.

An embodiment of determining the comparison threshold for the first level comparison from a given a priori address interval, in which case the non-first level comparison is achieved by a quartering method, will be described below with reference to the second multi-level comparison unit 1600 shown in fig. 16. The second multi-stage comparing unit 1600 shown in fig. 16 is similar to the second multi-stage comparing unit 1600 shown in fig. 14, except that the second multi-stage comparing unit 1600 shown in fig. 16 has more than one-stage comparator sub-units, i.e., five-stage comparator sub-units 1610 in total, but the number of comparators of the first-stage comparator sub-units is 1.

Furthermore, this embodiment differs from the embodiments described above in connection with fig. 14 and 11 in that the comparison threshold of the comparator 1611 in the first stage comparator subunit 1610 is set, for example, to V64, in accordance with the upper end of the a priori address interval described above (64 th address).

If the comparison result of the first-stage comparison is that the pulse energy is located in the prior address interval (in the low energy section), the amplitude of the pulse signal is between 0 and V64; the comparison thresholds of 3 comparators in the second stage comparator subunit may be set to V16, V32, V48 in a quartering manner; assuming that the pulse signal amplitude cannot cross the threshold V16, the pulse signal amplitude lies between 0 and V16; the comparison thresholds of 3 comparators in the third stage comparator subunit may be set to V4, V8, V12 in a quartering manner; assuming that the pulse signal amplitude cannot cross the threshold V4, the pulse signal amplitude lies between 0 and V4; the comparison thresholds of 3 comparators in the fourth stage comparator subunit may be set to V1, V2, V3 in a quartering manner; assuming that the pulse signal amplitude cannot cross the threshold V1, the pulse signal amplitude is between 0 and V1, i.e. at the 1 st energy address; if the pulse signal crosses V1 and cannot cross the threshold V2, the amplitude of the pulse signal is between V1 and V2, i.e. at the 2 nd energy track address; if the pulse signal crosses V2 and cannot cross the threshold V3, the amplitude of the pulse signal is between V2 and V3, i.e. at the 3 rd energy track address; if the pulse signal crosses V3, the amplitude of the pulse signal is between V3-V4, i.e., at the 4 th energy track. It can be seen that the energy addresses corresponding to the pulse amplitudes are determined by 4-level comparison.

In the example where the pulse energy of about 80% of the scintillation pulses corresponds to a track address below 64, only 1 first-stage comparison of 80% of the pulses is required.

If the comparison result of the first-stage comparison is that the pulse energy belongs to a high-energy section (namely, is outside the prior address interval), the amplitude of the pulse signal is between V64 and V256; the comparison thresholds of 3 comparators in the second stage comparator subunit may be set to V112, V160, V208 in a quartering manner; assuming that the pulse signal amplitude cannot cross the threshold V112, the pulse signal amplitude lies between V64-V112; the comparison threshold values of 3 comparators in the third-stage comparator subunit can be set as V76, V88 and V90 according to the quartering method, and the delayed pulse signals are input into the comparators; assuming that the pulse signal amplitude cannot cross the threshold V76, the pulse signal amplitude lies between V64-V76; the comparison threshold values of 3 comparators in the fourth-stage comparator subunit can be set as V67, V70 and V73 according to the quartering method, and the delayed pulse signals are input into the comparators; assuming that the pulse signal amplitude cannot cross the threshold V67, the pulse signal amplitude lies between V64-V67; the comparison threshold of 3 comparators in the fifth stage comparator subunit may be set to V65, V66, V67 in a quartering manner, if the pulse signal cannot cross V65, the amplitude of the pulse signal is between V64-V65, i.e. at the 65 th energy address; if the pulse signal crosses V65 and cannot cross the threshold V66, the amplitude of the pulse signal is between V65 and V66, i.e. at the 66 th energy track; if the pulse signal crosses V66 and cannot cross the threshold V67, the amplitude of the pulse signal is between V66 and V67, i.e., at the 67 th energy track. It can be seen that the energy addresses corresponding to the pulse amplitudes are determined by 5-level comparison.

In the example where the scintillation pulse has a pulse energy of about 80% and a corresponding address of less than 64, only about 20% of the pulses are located in the high energy segment (i.e., outside the a priori address interval), and only 1 first stage comparison of the pulses is required. Therefore, although the number of these scintillation pulses is 1 more, the effect of a significant reduction in the amount of comparison can be obtained for all the pulses to be measured.

It is contemplated that the multi-level comparison of the above embodiments may be accomplished by retrofitting the first multi-level comparison unit shown in fig. 10 or 12, for example by adding a one-way delay line.

In some embodiments, the given a priori address interval is 1, the comparison threshold of the first level comparison is 2 and is determined from the magnitude characterization values of the two end points of the a priori address interval, respectively.

In one example, the total energy track number is still n=m ⁿ For example (e.g., n=256), if a priori address interval is determined to be greater than the first address and less than the second address, e.g., 60 to 64 addresses, based on the pulse characteristics, then the comparison threshold of the first stage may be determined based on the priori interval. More specifically, the comparison threshold may be determined based on two end addresses (e.g., 60 and 64 addresses) of the a priori address interval, e.g., based on amplitude characteristic values corresponding to the 60 th and 64 th addresses, e.g., denoted as V60 and V64. It will be appreciated that the prior address interval may be set according to different pulse characteristics. For example, in pulsed neutron saturation logging, it is assumed that there is a significant The address corresponding to the pulse energy of the scintillation pulse corresponding to the gamma ray in part is between 60 and 64 addresses, so the a priori address interval is set to 60 to 64 addresses, and the comparison threshold of the first comparison is set to V60 and V64 as previously described.

An embodiment of determining the comparison threshold for the first level comparison from a given a priori address interval, in which case the non-first level comparison is achieved by a quartering method, will be described below by taking the second multi-level comparison unit 1700 shown in fig. 17 as an example. The second multi-stage comparing unit 1700 shown in fig. 17 is similar to the second multi-stage comparing unit 1600 shown in fig. 16, except that the number of comparators 1711, 1712 of the first-stage comparator subunit 1710 in the second multi-stage comparing unit 1700 shown in fig. 17 is 2.

If the comparison result of the first stage comparison is that the pulse energy is located in the prior address interval (called the middle energy section), namely the amplitude of the pulse signal is located between V60 and V64; the comparison threshold of 3 comparators in the second stage comparator subunit can be set to V61, V62, V63 in a quartering manner, if the pulse signal cannot cross V61, the amplitude of the pulse signal lies between V60-V61, i.e. at the 61 th energy address; if the pulse signal crosses V61 and cannot cross the threshold V62, the amplitude of the pulse signal is between V61 and V62, i.e. at the 62 th energy track; if the pulse signal crosses V62 and cannot cross the threshold V63, the amplitude of the pulse signal is between V62 and V63, i.e. at the 63 th energy track, and if the pulse signal crosses V63, the amplitude of the pulse signal is between V63 and V64, i.e. at the 64 th energy track. And 2-stage comparison is adopted to determine the energy address corresponding to the pulse amplitude.

The channel addresses corresponding to the pulse energy of the scintillation pulse of a significant part are all located in the prior channel address interval, and only two-stage comparison is needed in total, and the first-stage comparison of the pulse is needed for 2 times, so that the effect of remarkably reducing the comparison quantity can be obtained.

If the comparison result of the first level comparison is that the pulse energy is located outside the a priori address interval and in the high energy or low energy segment, then the address interval may be divided by a quarter method and compared with the embodiment described with reference to fig. 16. Correspondingly, the energy addresses corresponding to the pulse amplitudes are determined by adopting 4-level or 5-level comparison.

It is conceivable that the multi-level comparison of the above embodiment may be achieved by adapting the second multi-level comparison unit based on the dichotomy shown in fig. 15, for example by arranging the comparators of the first-level comparator subunit in two.

It is conceivable that the multi-stage comparison of the above embodiments may be achieved by adapting the first multi-stage comparison unit shown in fig. 8, 10, 12, for example by adding a delay line.

It is conceivable that in embodiments where a multi-level comparison is implemented, for example based on a delay line in combination with a comparator, the comparison threshold value adjacent to the a priori address interval is preferentially compared in a comparison of a subsequent level if the address interval determined by the first level comparison is outside the a priori address interval. This feature may bring the advantage of further reducing the amount of comparison, since even if pulses fall outside the a priori address interval, the number of pulses is greater the closer to the a priori address interval.

For example, taking a given a priori address interval as being less than 64 addresses, if the comparison result of the first stage comparison is that the pulse energy belongs to a high energy segment (i.e., outside the a priori address interval), the amplitude of the pulse signal is between V64 and V256, and the comparison thresholds of 3 comparators in the second stage comparator subunit may be set to V112, V160, and V208 according to the quartering method. If this example is implemented by a first multi-stage comparison unit based on delay lines in combination with comparators, then in the second stage comparison the comparison threshold V112, which is adjacent to the a priori address interval, i.e. adjacent to V64, is preferentially compared with the pulse signal from the line with the shorter delay (e.g. from the 2 nd delay line). This is to take into account that the likelihood of a pulse falling into V64-V112 is greater than the likelihood of falling into the other three address intervals.

In some embodiments, the given a priori address interval may be greater than or equal to 2 (M.gtoreq.2). Correspondingly, the comparison threshold of the first-stage comparison is 2M and is respectively determined according to the amplitude characterization values of the 2M endpoint addresses of the prior address interval.

In a further embodiment, when the pulse to be measured is a scintillation pulse generated by detecting a substance, in particular based on high energy radiation, the a priori energy address may be set based on the energy characteristics of the high energy radiation emitted by the substance component (element), such as the energy peak.

In a further embodiment, the substance constituent acquisition method further comprises determining M a priori address intervals based on the detected substance constituents. In some embodiments, the probe substance component may be a first component and a second component. In one particular embodiment, such as in logging applications, the probe material components are, for example, a carbon (C) component and an oxygen (O) component.

In some embodiments of the present invention, as shown in fig. 18, the determining M a priori address intervals specifically includes:

s1810: m energy windows are determined based on at least two components of the detected material. As previously described, the at least two components, for example, a first component and a second component, and in some embodiments, the first component energy window and the second component energy window may be determined from the first component and the second component. In one embodiment, for example, in performing a C/O spectroscopy, the two components, for example, a carbon (C) component and an oxygen (O) component, may be used to determine the nature of the downhole material based on the pulse count ratio over the energy range corresponding to each of the carbon element and the oxygen element on the resulting spectrum. Accordingly, the substance component obtaining method according to the preferred embodiment of the present application may be implemented based on the energy spectrum properties of the carbon element and the oxygen element.

Specifically, according to the precision requirements of different application scenes, according to prior information or according to the attributes of carbon and oxygen elements, the energy ranges of gamma rays generated by carbon atoms and oxygen atoms are respectively determined, and a carbon energy window and an oxygen energy window are obtained.

S1820: and determining the M priori address intervals corresponding to the M energy windows.

In some embodiments, step S1820 may include: determining M amplitude ranges corresponding to the M energy windows; and determining the M prior address intervals according to the determined M amplitude ranges.

In some embodiments, M amplitude ranges corresponding to the M energy windows may be determined in a manner similar to that described in step S110, such as determining the amplitude range corresponding to the first component energy window and determining the amplitude range corresponding to the second component energy window.

In one particular embodiment, for example, in performing C/O spectroscopy, a C pulse amplitude range corresponding to a C energy window and an O pulse amplitude range corresponding to an O energy window may be determined.

In a specific example, pulses generated by a large number of gamma photons can be collected at a sampling frequency as high as possible through high-speed sampling equipment such as an oscilloscope, pulse data are processed to obtain energy information and voltage peak value information of each pulse, a scatter diagram is drawn and fitted by the energy and the peak value of the pulse, and a linear mapping relation between the energy and the peak value can be obtained theoretically.

In further specific examples, M amplitude ranges corresponding to M energy windows may be interpolated from a look-up table between energy and peak values.

In another embodiment, when the address is an energy address, step S1820 may determine a priori address intervals corresponding to M energy windows directly according to the energy windows and the energy characterization values corresponding to the energy addresses, and determine the amplitude ranges corresponding to the priori address intervals accordingly.

For example, in one embodiment, after determining the C pulse amplitude range corresponding to the C energy window and the O pulse amplitude range corresponding to the O energy window, a plurality of comparison thresholds of the first-stage comparison in the multi-stage comparison may be set accordingly with reference to the foregoing, and after performing the first-stage comparison, the comparison threshold of the subsequent-stage comparison may be dynamically adjusted according to the address interval in which the pulse to be measured falls, which is not described herein.

Furthermore, in the preferred embodiment, the carbon to oxygen ratio (C/O ratio) for C/O spectroscopy can be further obtained on a pulse digitization basis, i.e., on a spectrum basis of all pulses.

Here, in the embodiment shown in fig. 19, the substance component obtaining method further includes:

s1910: determining counts of the scintillation pulses falling within a first component energy window and a second component energy window, respectively; and

S1920: a ratio of the first component to the second component is determined based on the count.

In a specific embodiment, such as in performing C/O spectroscopy, the carbon to oxygen ratio may be determined by a carbon to oxygen ratio determination unit that is independent of the trace site determination unit, as shown in fig. 20.

In the embodiment shown in fig. 20, the carbon-oxygen ratio determination unit 2000 includes a first carbon comparator 2011, a second carbon comparator 2012, a first oxygen comparator 2021, a second oxygen comparator 2022, a carbon counter 2030, an oxygen counter 2040, a calculation unit 2050, and an optional correction unit 2060.

Thus, in this embodiment, as shown in fig. 21, the step S1910 may include:

s2110: determining whether the scintillation pulse falls into an amplitude range corresponding to the first component energy window or an amplitude range corresponding to the second component energy window according to comparison of the amplitude of the scintillation pulse and the amplitude range;

s2120: performing first component counting on scintillation pulses falling into an amplitude range corresponding to a first component energy window; and

s2130: the scintillation pulses falling within the amplitude range corresponding to the second component energy window are second component counted.

Specifically, the pulse to be detected is input into a first carbon comparator, a second carbon comparator, a first oxygen comparator and a second oxygen comparator in parallel, the first carbon comparator sets a comparison threshold value based on the lower limit of the amplitude range corresponding to the C energy window, and the second carbon comparator sets the comparison threshold value based on the upper limit of the amplitude range corresponding to the C energy window; the first oxygen comparator sets a comparison threshold based on a lower limit of the amplitude range corresponding to the O energy window, and the second oxygen comparator sets a comparison threshold based on an upper limit of the amplitude range corresponding to the O energy window.

In some embodiments, the carbon counter connects the first carbon comparator and the second carbon comparator; the oxygen counter is connected with the first oxygen comparator and the second oxygen comparator; the calculating unit is connected with the carbon counter and the oxygen counter and is used for calculating the carbon-oxygen ratio.

An optional correction unit 2060 is connected to the negative terminals of the first carbon comparator 2011, the second carbon comparator 2012, the first oxygen comparator 2021, and the second oxygen comparator 2022 for setting a correction threshold.

Here, the C pulse amplitude range corresponding to the C energy window and the O pulse amplitude range corresponding to the O energy window may be determined in the step S1820 as described above, for example, according to a linear mapping relationship or a lookup table, or according to an amplitude range determined according to the determined a priori address interval. Thereby, four pulse amplitude (peak value) end point values corresponding to the carbon energy window end point and the oxygen energy window end point, respectively, can be obtained, for example, in V _Cmin ,V _Cmax ,V _Omin ,V _Omax And (3) representing.

The comparison thresholds of the first carbon comparator 2011, the second carbon comparator 2012, the first oxygen comparator 2021 and the second oxygen comparator 2022 can be set to the four pulse peak end values V by digital-to-analog converters _Cmin ,V _Cmax ,V _Omin ,V _Omax . Thus, when the pulse under test enters the system, the pulse under test is input into the four comparators in parallel, if the pulse under test passes V _Cmin Without crossing V _Cmax The carbon counter is incremented by 1, if the pulse to be measured passes V _Omin Without crossing V _Omax The oxygen counter is incremented by 1 and neither counter needs to respond if both are not met.

When all the pulses to be measured pass through the system, the values of the two counters can be read and calculated by the calculation unit, and then the C/O value can be obtained.

As previously described, the present embodiment also optionally includes the step of calibrating the first carbon comparator 2011, the second carbon comparator 2012, the first oxygen comparator 2021, the second oxygen comparator 2022 described above.

In an actual logging scene, the equipment needs to operate in an environment with temperature change and general high temperature, and the temperature is often a non-negligible factor influencing the working state of an electronic device, in order to enable an instrument to still obtain more accurate data in a downhole process, a correction unit can be arranged for a DAC, if one DAC channel is additionally arranged as an input of the correction unit, the correction unit can know the output difference of the DAC at different temperatures according to prior information, and accordingly, the comparison thresholds of four comparators are corrected correspondingly. For example, taking a DAC for setting the amplitude end point as an example to set the comparison threshold value, such as 3V, when the comparison threshold value is deviated due to a temperature change, such as a deviation value of 0.5V, the deviation comparison threshold value, such as-0.5, may be set by the correction unit, such as the correction DAC, thereby correcting the deviation of the carbon comparator and the oxygen comparator.

In the preferred embodiment, on the basis of determining the energy channel address (such as based on a multi-stage dichotomy or a quartering method) of each pulse to be detected, the carbon-oxygen ratio energy spectrum is determined by additionally arranging the carbon/oxygen comparator, so that the spectrum forming time of the carbon-oxygen ratio energy spectrum is effectively shortened.

In an alternative preferred embodiment, it is also conceivable to obtain the carbon-oxygen ratio by counting the pulse count in the address or address interval corresponding to the energy window C and the pulse count in the address or address interval corresponding to the amplitude range corresponding to the energy window O.

Thus in this embodiment, after determining the energy information of all the pulses to be measured on all the addresses in step S150, for example, after generating the energy spectrum of all the energy addresses, the counts falling into the C energy window and the O energy window respectively may be determined from the energy addresses corresponding to the C energy window and the O energy window. For example, the C energy window corresponds to the A-B address and the O energy window corresponds to the C-D address, where only counts within the two address intervals need to be calculated for determining the carbon to oxygen ratio.

Further, as described further below, embodiments of the present application also relate to a scintillation pulse-based material composition determination method that is independent of or in combination with the material composition acquisition method of embodiments of the present application.

In further embodiments, the comparison of the amplitude magnitudes of the plurality of pulses to be measured and the amplitude characterization values of the plurality of addresses may be achieved by a single stage comparison.

In the embodiment shown in fig. 22, an embodiment of a single stage comparison is shown. Specifically, step S140 may include:

s2210: subjecting the amplitude of each pulse to be measured to a single-stage comparison comprising a plurality of comparisons corresponding to the number of addresses of the plurality of addresses to determine the address in which the pulse to be measured falls; and

s2220: and determining the address of the channel where the pulse to be detected falls according to the comparison result of the single-stage comparison.

To achieve the single-stage comparison described above, the address determination unit may comprise or may be a single-stage comparison unit.

In some embodiments, the plurality of comparisons in the module architecture of the single-stage comparison unit for implementing the single-stage comparison may be implemented by a plurality of comparators, wherein the number of the plurality of comparators is greater than or equal to the number of the plurality of addresses.

In further embodiments it is also possible to implement a comparator architecture with fewer addresses, even a single comparator architecture, for example by combining different delays of the delay lines with adjustable comparators.

An exemplary embodiment of a first single stage comparison unit 2300 for achieving single stage comparison is shown in fig. 23. The first single stage comparison unit 2300 includes a plurality of parallel delay lines 2310 coupled to the pulse inputs to be measured, an adjustable comparator 2320 coupled to the delay lines, and an arbiter 2330 operatively coupled to the adjustable comparator. Preferably, the delay times of at least some of the delay lines are different, and in the embodiment shown in fig. 23, the delay times of each delay line are different. Preferably, the number of the plurality of parallel delay lines is greater than or equal to the number of the plurality of addresses. In the illustrated embodiment, N parallel delay lines 2310 are shown.

For example, the total energy address number is n=256, where the number of N parallel delay lines 2310 corresponds to the total energy address number. Therefore, the address of the pulse to be detected can be determined by adopting a single-stage N-level method, and the comparison times in the single-stage comparison are the same as the number of energy addresses.

Specifically, the input pulse can be input into the comparator after passing through 256 delay lines with different delays, namely pulse signals are repeatedly input into the positive input end of the comparator for 256 times, the threshold voltage of each comparison is set by the arbiter, the arbiter sequentially assigns comparison thresholds for the negative input end of the comparator according to the amplitude representation value corresponding to the energy spectrum channel address, such as V1, V2, V3, … … and V256, and the specific channel address to which the energy of the input pulse to be detected belongs can be obtained after 256 times of comparison.

The embodiment simplifies a dynamic threshold value spectrum forming scheme adopting multi-level comparison, and only sets one-level comparison, compared with the dynamic threshold value spectrum forming scheme setting multi-level comparison, the embodiment can reduce or avoid errors caused by differences among comparators to a certain extent. By way of explanation and not limitation, in a dynamic threshold spectral scheme where multiple levels of comparisons are provided to compare input pulses, errors may be introduced in the comparison of the pulse peaks due to comparator differences, which ultimately may affect the accuracy of the resulting energy spectrum.

As previously described, in some embodiments, multiple comparisons in a module architecture of a single-stage comparison unit for implementing a single-stage comparison may be implemented by multiple comparators.

Although not shown in the figure, it is conceivable to provide N parallel comparators greater than or equal to the number of energy addresses, preferably the same number of comparators as the number of energy addresses.

For example, taking the total address number as 256 channels as an example, 256 comparators connected in parallel are provided, for example, the corresponding DACs provide amplitude representing values corresponding to energy addresses (such as end points of pulse peak intervals corresponding to energy addresses) for each comparator as comparison thresholds.

As described above, in the embodiment of the present application, the address interval in which each pulse to be measured falls may also be predetermined based on the time parameter.

In a further embodiment, the over-threshold time (Time Over Threshold, TOT for short) may be used in conjunction with a dynamic comparison threshold to count the addresses that pulses, such as scintillation pulses, fall into.

In a specific embodiment, as shown in fig. 24, the step S140 may include:

s2410: mapping relation data of threshold time and energy range of multiple reference pulses is provided.

In a specific embodiment, the threshold-time-energy-range mapping data is a threshold-time-energy-range lookup table.

In some embodiments, the plurality of reference pulses of step S2410 are the plurality of reference pulses described in step S110 or a portion thereof, or the plurality of reference pulses in step S2410 and step S110 partially overlap each other.

In further preferred embodiments, the plurality of pulses of step S2410 are reference pulses different from those described in step S110, such as the reference pulses described in step S110 or other acquired pulses.

Here, a lookup table of pulse energy ranges corresponding to TOTs may be obtained based on a priori information.

For example, the comparator may be provided with a comparison threshold slightly greater than the maximum amplitude of noise, e.g. a threshold voltage V _t1 A number of pulses of known energy are passed through the channel, the time value at which each pulse crosses the threshold, i.e. the threshold time (TOT), is recorded, and a priori information is available, e.g. at the threshold voltage V _t1 And a pulse energy range lookup table corresponding to TOT. In addition or in lieu of this, the comparator can also be provided with other comparison thresholds, such as a threshold voltage V _t2 、V _t3 Etc., and accordingly obtain the over-threshold time (TOT) at these comparison thresholds, e.g., threshold voltages. Thus, based on a priori information, the correspondence of TOT to energy range can be obtained.

By way of explanation and not limitation, since pulse widths of pulse signals differ little and if the pulses are shaped, the pulse widths of the shaped pulses may be more similar, the TOT of the pulse signals crossing the threshold voltage differ little, resulting in the same TOT potentially corresponding to multiple pulse energies, i.e., a range of energies.

S2420: at least one threshold time of the pulse to be detected is obtained, and each threshold time corresponds to an amplitude threshold.

As previously described, step S140 may be implemented by the track address determination unit. Fig. 26 and 28 illustrate an address determination unit 2600, 2800 that may be used to implement the embodiment shown in fig. 24, including, inter alia, a more threshold time unit that connects pulse inputs to be measured.

As shown in fig. 26, the address determining unit 2600 may include a comparing unit 2610 connected to the pulse input to be measured, a threshold-crossing time unit 2630 connected to the pulse input to be measured, and an arbiter 2620 operatively connected to the threshold-crossing time unit 2630 and the comparing unit 2610.

In the embodiment shown in fig. 26, the comparison unit 2610 comprises a physical multi-stage comparator subunit 2611, each stage comparator subunit 2611 comprising a single physical adjustable comparator which can perform, for example, a binary comparison in a subsequent single stage or multi-stage comparison. It will be appreciated that the comparison unit shown in fig. 26 may be configured or adapted with reference to the single or multi-stage comparison unit configuration described in other embodiments of the present application, such as the comparison unit configurations shown in fig. 8, 10, 12-17, 23. In particular, the comparison unit shown in fig. 26 may include a physical multi-stage comparator subunit when used to implement multi-stage comparison, or may include a plurality of parallel delay lines for implementing multi-stage comparison with different delays and an adjustable comparator connected to the delay lines, all falling within the scope of the present application.

With continued reference to fig. 26, the threshold time over unit 2630 may include a threshold time over comparator 2631 and a threshold Time Over (TOT) acquisition processor 2634 coupled to the threshold time over comparator 2631.

Referring to fig. 26 and 27 in combination, the threshold crossing time comparator 2631 may set a comparison threshold, here an amplitude threshold, such as a voltage threshold V _t1 . Accordingly, by inputting the pulse under test 2710 to the threshold-crossing time comparator 2631, the threshold-crossing time comparator 2631 will output a transition signal 2720, such as from low level 0 to high level 1 and from high level 1 to low level 0, as the pulse under test crosses the amplitude threshold, including from bottom to top and from top to bottom. Accordingly, the time of generating the transition signal, e.g., t, may be determined by a time determining unit, e.g., TDC ₁ And t ₂ . Thus, the TOT acquisition processor 2634 may determine that it is from the same sourceA threshold time-crossing comparator 2631 for time interval between two transition moments, e.g. t ₂ -t ₁ To determine the threshold value at the amplitude, e.g. voltage threshold value V _t1 TOT below.

In further embodiments, multiple TOTs may be determined from multiple amplitude thresholds.

As shown in fig. 28, the address determining unit 2800 may include a comparing unit 2810 connected to the pulse input to be measured, a threshold time unit 2830 connected to the pulse input to be measured, and an arbiter 2820 operatively connected to the threshold time unit 2830 and the comparing unit 2810.

With continued reference to fig. 28, the threshold time over unit 2830 may include a plurality (e.g., 3) threshold time over comparators 2831 and a threshold Time Over (TOT) acquisition processor 2834 connected to the threshold time over comparators 2831.

The threshold time unit 2830 shown in fig. 28 differs from the threshold time unit 2630 shown in fig. 26 in that the threshold time unit 2830 includes a plurality (e.g., 3) threshold time comparators 2831, which may set different comparison thresholds, in this case amplitude thresholds, such as voltage threshold V _t1 、V _t2 、V _t3 . Thus, in the embodiment shown in FIG. 28, a plurality (e.g., 3) TOTs may be determined from a plurality of magnitudes.

S2430: and determining a first address interval according to the at least one threshold crossing time of the pulse to be detected and the mapping relation data of the threshold crossing time and the energy range.

In this embodiment, the address is an energy address.

Thus, the mapping relationship data, such as a lookup table, may be provided based on the step S2410, and the energy range corresponding to the TOT determined in the step S2420 may be determined, and then the first address interval corresponding to the TOT, which may be referred to herein as the TOT address interval, may be determined based on the energy characterization value corresponding to the energy address set in the step S120.

In one particular example, a comparison threshold, such as a threshold voltage, of the threshold time over comparator 2631 may be set to V by the arbiter 2620 and/or the TOT acquisition processor 2634 _t1 . To be measuredThreshold V is crossed after pulse input by threshold time comparator 2631 _t1 The TOT acquisition processor 2634 determines the TOT value of the pulse signal crossing the threshold, and the arbiter 2620 determines the range of pulse energy corresponding to the TOT value according to the obtained lookup table, thereby determining the first address interval corresponding to the TOT, for example, the two end energy values of the energy range are corresponding to two energy addresses, and the energy interval between the two energy addresses is the first address interval reduced relative to the total address number. More specifically, the threshold time comparator 2631 compares a threshold value, such as a threshold voltage V _t1 For example, a threshold voltage slightly greater than the maximum amplitude of the noise. According to the determined threshold time value (TOT value) of the pulse to be measured, the energy range corresponding to the TOT value, such as range [3.48MeV,3.66MeV ] can be obtained by looking up the table]And further determining that the two energy values are located at the 100 th energy track address and the 105 th energy track address, respectively, whereby the determined energy track address interval is the 100 th to 105 th energy track address.

As previously described, a plurality of TOTs may be determined according to a plurality of amplitude thresholds in step S2420, and accordingly, a first address interval (TOT address interval) may be determined according to the energy ranges corresponding to the plurality of TOTs in step S2430, for example, by an intersection and/or a subset of the energy ranges corresponding to the plurality of TOTs. In the particular embodiment shown in FIG. 28, the voltage threshold V may be based on multiple (e.g., 3) voltage thresholds _t1 、V _t2 、V _t3 An intersection of the determined energy ranges for a plurality (e.g., 3) of TOTs is determined to determine a first address interval (TOT address interval). In a specific example, for example, voltage threshold V _t1 The energy address range corresponding to the determined TOT is from the 100 th energy address to the 120 th energy address, and the voltage threshold V _t2 The energy address range corresponding to the determined TOT is from the 90 th energy address to the 110 th energy address, and the voltage threshold V _t3 The energy address interval corresponding to the determined TOT is from the 88 th energy address to the 105 th energy address, and the final first address interval (TOT address interval) can be determined as the 100 th to 105 th energy address according to the energy range or the intersection of the energy address intervals.

S2440: the amplitude of each pulse to be measured is subjected to single-stage comparison or multi-stage comparison to determine the second address interval in which the pulse to be measured falls.

In an embodiment of the present application, each level of comparison defines at least two second address intervals by at least one comparison threshold, and the comparison threshold of the single level comparison or the first level comparison threshold of the multi-level comparison is determined from the first address intervals.

S2450: and determining the address of the channel where the pulse to be detected falls according to the single-stage or multi-stage comparison result.

The first address interval (TOT interval) determined according to the aforementioned step S2430 may be used to dynamically determine a comparison threshold for a subsequent single-stage or multi-stage comparison. The comparison method described in this embodiment may be, for example, a single-stage or multi-stage comparison method as described in other embodiments. In some embodiments, the comparison may be based on a single or multiple parallel adjustable comparators. In other embodiments, the comparison may be based on a combination of a delay line and an adjustable comparator.

For example, the 100 th to 105 th energy addresses are taken as an example, because the number of the addresses in the first address interval is smaller, the addresses can be directly compared, for example, the middle energy address can be determined to be the 102 th energy address, for example, the amplitude of the pulse signal passes through the amplitude representation value corresponding to the 102 th energy address and is positioned in the 103 th to 105 th energy addresses, the amplitude representation value corresponding to the 104 th energy address is taken as a comparison threshold, the energy address is positioned in the 105 th energy address when the amplitude representation value is larger than the comparison threshold, the energy address is positioned in the 103 th to 104 th energy addresses when the amplitude representation value is smaller than the comparison threshold, the amplitude representation value corresponding to the 103 th energy address is taken as the comparison threshold, the pulse signal passes through the comparison threshold and is positioned in the 104 th energy address, and otherwise the pulse signal is positioned in the 103 th energy address.

Alternatively to the embodiment shown in fig. 24, the first address interval may be dynamically predetermined according to preset criteria. In a specific embodiment, referring to fig. 25, the step S140 may include:

s2510: threshold-crossing time-energy range mapping relationship data for a plurality of reference pulses is provided.

In step S2510, reference may be made to step S2410 described in the embodiment illustrated in fig. 24.

As shown in fig. 25, the step S140 further includes performing the following steps:

s2520: a threshold value of the amplitude value is set,

s2530: acquiring the threshold time of the pulse to be detected, wherein the threshold time corresponds to the set amplitude threshold,

s2540: determining or updating a first address interval according to the threshold crossing time and the threshold crossing time-energy range mapping relation data of the pulse to be tested, and

s2550: judging whether the preset standard is met.

If yes, the loop is exited, and if not, the loop step is continuously executed.

In some embodiments, the above-described steps of loop execution may be implemented using the track address determination unit 2800 shown in fig. 28. As previously described, the threshold time over unit 2830 may include a plurality (e.g., 3) threshold time over comparators 2831 and a threshold Time Over (TOT) acquisition processor 2834 connected to the threshold time over comparators 2831.

Accordingly, the threshold-crossing time comparators are plural, and the plural threshold-crossing time comparators set different amplitude thresholds from each other.

In some embodiments, the predetermined criterion is that the set amplitude threshold reaches a predetermined number. For example, when the set amplitude threshold is 3 or more, the loop is exited, and the subsequent steps are performed according to the newly determined first address section.

In other embodiments, the predetermined criterion is that addresses within the first address interval are less than a predetermined number. For example, when the number of addresses within the first address interval is small, such as less than 5, the loop may be exited and subsequent steps may be performed based on the newly determined first address interval.

After exiting the loop, the step S140 may further include:

s2560: the amplitude of each pulse to be measured is subjected to single-stage comparison or multi-stage comparison to determine the second address interval in which the pulse to be measured falls.

In a specific embodiment, each level of comparison defines at least two second address intervals by at least one comparison threshold, and the comparison threshold of the single level comparison or the first level comparison threshold of the multi-level comparison is determined from the first address intervals.

S2570: and determining the address of the channel where the pulse to be detected falls according to the single-stage or multi-stage comparison result.

Similar to step S2450, the comparison method described in step S2570 may be, for example, a single-stage or multi-stage comparison method as described with reference to other embodiments. In some embodiments, the comparison may be based on a single or multiple parallel adjustable comparators. In other embodiments, the comparison may be based on a combination of a delay line and an adjustable comparator.

In the embodiments shown in fig. 24 to 28, by counting the channel address where the pulse, such as the scintillation pulse, falls by using the threshold crossing time (Time Over Threshold, referred to as TOT for short) in combination with the dynamic comparison threshold, the method has advantages in the application scenario of drawing the high-precision energy spectrum, can effectively shorten the time for forming the spectrum, and changes the sequence of the voltage compared with the pulse, so that the acquisition of the comparison result is accelerated as a whole. Further, in the embodiment shown in fig. 25 or fig. 25 in combination with fig. 28, the energy address range is pre-screened, so that the spectral efficiency is further improved, and the comparison time is effectively reduced.

Continuing back to fig. 1, the substance component obtaining method 100 may further include step S150: and obtaining the energy information of the pulses to be detected according to the pulse count to be detected in each address and the amplitude-energy mapping relation data or the energy representation value of the energy address.

More specifically, step S150 includes: and generating energy spectrums of the plurality of pulses to be detected.

In some embodiments, when the address set in step S120 is an energy address, the energy spectrum may be obtained by drawing a histogram based directly on the counted scintillation pulse count in each energy address.

In an alternative embodiment, when the address set in step S120 is an amplitude address, the amplitude distribution may be obtained based on the count of scintillation pulses counted in the amplitude address, for example, by plotting a histogram. Next, the energy range corresponding to each amplitude address may be determined from amplitude-energy mapping data, such as an amplitude-energy look-up table, and the amplitude distribution converted accordingly into energy information, such as an energy spectrum.

In the embodiment of the present application, before counting the pulse to be detected, step S2930 of threshold correction is further included.

Alternatively, when the set address is the energy address, as shown in fig. 29, the substance component obtaining method may further include a correction step S2930 of: correcting amplitude representative values of a plurality of energy addresses relative to energy representative values of the plurality of energy addresses.

It will be appreciated that steps S2910, S2920, S2940 and S2950 in the embodiment shown in fig. 29 may refer to steps S110, S120, S140 and S150 in the embodiment shown in fig. 1, respectively, and are not described herein.

In the embodiment shown in fig. 30, the step S2930 may include:

s3010: determining the energy addresses corresponding to the first correction pulses according to the comparison results of the amplitude values of the first correction pulses and the amplitude characterization values of the energy addresses;

s3020: generating an energy spectrum of the first correction pulse according to the first correction pulse count in each energy address and the energy characterization value of the energy address, wherein the energy spectrum of the first correction pulse has a first characteristic peak value;

s3030: setting a plurality of first correction energy addresses;

the energy ranges corresponding to the plurality of first correction energy addresses are smaller than the energy ranges corresponding to the plurality of energy addresses, and each correction energy address has a respective energy representation value and a magnitude representation value which is correspondingly determined according to the magnitude-energy mapping relation data;

s3040: determining the correction energy addresses corresponding to the plurality of second correction pulses according to the comparison results of the amplitude magnitudes of the plurality of second correction pulses and the amplitude characterization values of the plurality of first correction energy addresses;

s3050: generating an energy spectrum of a second correction pulse according to the second correction pulse count in each first correction energy track address and the energy representation value of the correction energy track address, wherein the energy spectrum of the second correction pulse has a first correction characteristic peak value; and

S3090: correcting the energy or amplitude characterization values of the plurality of energy addresses based on a first difference between the first characteristic peak and the first corrected characteristic peak.

In some embodiments, correction of the energy addresses may be achieved by setting different address divisions. This can be achieved by setting different modes of operation. One such correction mode, for example, is a normal mode of operation or a mode similar to the normal mode of operation, in which a "normal" energy track address, also referred to as the energy track address to be corrected, is used for the pulse to be measured. Other correction modes that may be used may be performed at corrected energy addresses having energy ranges less than the "normal" energy addresses. For convenience of distinction, the former may be referred to as a first correction mode, and the latter may be referred to as a second correction mode.

In some embodiments of the present application, the correction step uses a single characteristic peak. A specific example of performing correction using a single characteristic peak will be described below in connection with the embodiment shown in fig. 30.

Specifically, as shown in steps S3010 and S3020, the method of digitally acquiring energy information as described above may be operated in the first correction mode similar to the normal operation mode. The energy spectrum of 256 energy channel addresses with the characterizable energy range within 9MeV can be obtained by normal operation of the energy spectrum in a working environment required, and a characteristic peak (a peak formed by pulses formed by gamma photons generated by H (hydrogen) atoms, hereinafter referred to as H peak) which can be clearly identified can be arranged on a low energy section of the energy spectrum, so that a corresponding first characteristic peak is obtained. Optionally, the channel address E corresponding to the H peak on the energy spectrum obtained by working in the first correction mode can be obtained _H1 。

In some embodiments, in step S3030, the plurality of first correction energy addresses may be set according to the first characteristic peak value, so that the first characteristic peak value falls within an energy range corresponding to the first correction energy address.

In a further embodiment, in step S3030, the plurality of first correction energy addresses may be set according to the first characteristic peak value and a preset shrinkage ratio, so as to shrink energy ranges corresponding to the plurality of energy addresses according to the preset shrinkage ratio, thereby obtaining energy ranges corresponding to the plurality of first correction energy addresses, and make the first characteristic peak value fall within the energy ranges corresponding to the first correction energy addresses.

In a further embodiment, in step S3030, the first characteristic peak is an energy range median corresponding to the first correction energy track address.

In a further embodiment, in step S3030, the number of corrected energy addresses may correspond to the number of energy addresses to be corrected, for example, all 256 tracks.

The following description continues with specific embodiments of steps S3030 to S3050, for example, may be set to a second correction mode, where the underlying logic of the system operation is the same as the logic of the first correction mode similar to the normal operation mode, but different in that, in the second correction mode, the energy ranges corresponding to the plurality of first correction energy addresses are smaller than the energy ranges corresponding to the plurality of energy addresses to be measured. For example, referring to the specific example described above, the energy ranges for the plurality of first correction energy addresses are no longer the original 0 to 9mev, but are determined with the first characteristic peak and the predetermined contraction ratio. For example, the shrinkage ratio is 1/10 in the 900keV energy range centered around the first characteristic peak of 2.25MeV, i.e., 1.8MeV to 2.7 MeV. Correspondingly, the center of the energy range corresponding to the first correction energy track addresses is the theoretical energy value of 2.25MeV of the H peak, and the range size is 900keV which is the integral tenth of the original range of 0-9 MeV. The number of energy addresses is still 256. Correspondingly, the current energy range of 1.8 MeV-2.7 MeV can be equally divided into 256 parts, and according to the range, the energy (representing value) corresponding to each channel address on the energy spectrum is re-divided, namely, the corresponding pulse peak value or maximum amplitude representing value is searched according to the energy corresponding to each channel address. At the position of In this way, the method for digitally acquiring energy information described above can be operated in a second correction mode, which results in a more accurate energy spectrum with a narrower energy range. The energy range of the energy spectrum corresponding to the first correction energy channel address comprises the region where the H peak is located, and a more accurate energy value (namely a first correction characteristic peak value) where the H peak is located can be obtained through the energy spectrum, and the first correction channel address E of the H peak at the moment is recorded _H2 。

Subsequently, as described in step S3090, the energy or amplitude characterization values of the plurality of energy addresses may be corrected based on a first difference between a first characteristic peak and the first corrected characteristic peak

As an example, it can be determined that in the first correction mode similar to the normal operation mode, the energy corresponding to the H peak is 9 XE _H1 256 MeV (noted Energy _H1 ) While in the second correction mode the energy corresponding to the H peak is (1.8+0.9XE) _H2 /256) MeV (noted Energy _H2 ) (the range is 1.8MeV to 2.7MeV, in which the addresses are arranged from 0 to 255, so that the initial value of 1.8MeV is added), the ratio of H peak occurrence is obtained with the difference of k=energy _H1 /Energy _H2 。

In the embodiment shown in fig. 30, the correction can be performed by using the linear function y=kx, so that the energy value represented by each energy track in the first correction mode similar to the normal operation mode should be 1/k times the original energy value, i.e. the energy value represented by each energy track in the normal operation mode for the pulse to be measured in the subsequent operation mode should be 1/k times the original energy value. Different forms of correction can be made accordingly. In one embodiment, the energy characteristic value corresponding to the energy track address to be corrected can be adjusted to be 1/k times the original value. In another embodiment, the amplitude characterization value corresponding to the energy track address to be corrected can be adjusted to k times the original value. For example, the voltage threshold corresponding to the energy address to be corrected is adjusted to k times of the original voltage threshold. The relative correction of the energy representation value and the amplitude representation value of the energy track address is completed so as to reduce the degree of energy spectrum deviation.

It will be appreciated that more than one characteristic peak may be used for correction. Accordingly, the correction function includes, but is not limited to, a linear function y=kx, and the accuracy of the correction can also be improved by increasing the characteristic peak value used for the correction and the parameter or the number of times in the corresponding function model.

In the embodiment shown in fig. 31, the step S2930 may include:

S3110: determining the energy addresses corresponding to the first correction pulses according to the comparison results of the amplitude values of the first correction pulses and the amplitude characterization values of the energy addresses;

s3120: generating an energy spectrum of the first correction pulse according to the first correction pulse count in each energy address and the energy characterization value of the energy address, wherein the energy spectrum of the first correction pulse has a first characteristic peak value and a second characteristic peak value;

s3130: setting a plurality of first correction energy addresses;

s3140: determining the correction energy addresses corresponding to the plurality of second correction pulses according to the comparison results of the amplitude magnitudes of the plurality of second correction pulses and the amplitude characterization values of the plurality of first correction energy addresses;

s3150: generating an energy spectrum of a second correction pulse according to the second correction pulse count in each first correction energy track address and the energy representation value of the correction energy track address, wherein the energy spectrum of the second correction pulse has a first correction characteristic peak value;

S3160: setting a plurality of second correction energy addresses;

the energy ranges corresponding to the plurality of second correction energy addresses are smaller than the energy ranges corresponding to the plurality of energy addresses, and each second correction energy address has a respective energy representation value and an amplitude representation value which is correspondingly determined according to the amplitude-energy mapping relation data;

s3170: determining second correction energy addresses corresponding to the third correction pulses according to comparison between the amplitude values of the third correction pulses and the amplitude characterization values of the second correction energy addresses;

s3180: generating an energy spectrum of a third correction pulse according to a third correction pulse count in each second correction energy track address and an energy representation value of the second correction energy track address, wherein the energy spectrum of the third correction pulse has a second correction characteristic peak value; and

s3190: correcting the energy or amplitude characterization values of the plurality of energy addresses based on a first difference between the first characteristic peak and the first correction characteristic peak and a second difference between the second characteristic peak and the second correction characteristic peak.

In the embodiment shown in fig. 31, steps S3110 to S3140 may refer to steps S3010 to 3040.

In step S3150, the energy spectrum of the first correction pulse also has a second characteristic peak. Accordingly, the second correction feature peak value may be acquired in steps S3160 to 3180. Further, the energy track address will be corrected based on the difference of the two characteristic values and the correction values thereof in step S3190.

Accordingly, in the embodiment shown in fig. 31, in step S3170, the plurality of second correction energy addresses may be set according to the second characteristic peak value such that the second characteristic peak value falls within an energy range corresponding to the second correction energy address.

In a further embodiment, in step S3170, the plurality of second corrected energy addresses may be set according to the second characteristic peak value and a preset shrinkage ratio, so as to shrink the energy ranges corresponding to the plurality of energy addresses according to the preset shrinkage ratio, thereby obtaining the energy ranges corresponding to the plurality of second corrected energy addresses, and make the second characteristic peak value fall within the energy ranges corresponding to the second corrected energy addresses.

In a further embodiment, in step S3170, the second characteristic peak is an energy range median corresponding to the second correction energy track address.

In a further embodiment, in step S3170, the second correction energy track number may correspond to the energy track number to be corrected, for example, all 256 tracks.

As an example, when y=kx+b, y=ax is used ² When the functions are selected as corrected mathematical models, two unknown parameters in the models can be obtained by solving two corresponding sets of data.

Since two correction operation modes similar to the second correction operation mode described above can be set. Accordingly, there may be a first corrective operation mode, similar to the normal operation mode, and second and third corrective operation modes. For example, the second correction mode may also be referred to as an H correction mode, and the third operation mode added thereto may be referred to as a C correction mode (a peak composed of pulses formed by gamma photons generated by C atoms, hereinafter referred to as a C peak). Similar to the H correction mode, in the C correction mode, an Energy range with a second characteristic peak, such as C peak (4.43 MeV), as a range of 900keV is used as the Energy range corresponding to a plurality of second correction Energy track addresses, and the Energy corresponding to the C peak is recorded as Energy _C2 Meanwhile, the Energy corresponding to the C peak obtained in the first correction working mode similar to the normal working mode is recorded as Energy _C1 Will (Energy) _C2 ，Energy _C1 )，(Energy _H2 ，Energy _H1 ) Substituting the obtained value in the form of (x, y) into the determined function model to obtain the unknown parameter, obtaining the expression y=f (x) of the function, setting the amplitude characterization value before correction, such as the threshold voltage, as V as E=g (V) is a certain function relation between the pulse peak value and the pulse energy ₁ And V before correction ₁ Theoretically corresponding to energy (characterization value) of spectrum E ₁ Actual V ₁ The corresponding energy value should be E ₂ It can be seen that E ₂ =g(V ₁ ) And E is ₁ =f(E ₂ ) The method comprises the steps of carrying out a first treatment on the surface of the The threshold voltage after correction is V ₂ Corrected V ₂ The energy on the corresponding energy spectrum is E ₁ I.e. E ₁ =g(V ₂ ) So g (V) ₂ )=f(E ₂ )=f(g(V ₁ ) V), i.e ₂ =g ^-1 (f(g(V ₁ )))。

Although embodiments are shown herein in which correction is based on one or two characteristic peaks, parameters in the mathematical model may be further increased, if desired, while the number of characteristic peaks used for correction is increased. For example, the characteristic peak of a certain element can be taken again, the accurate energy spectrum is obtained, and the steps are repeated to realize correction.

Compared with the traditional MVT method which is suitable for sampling known pulses, the threshold value is determined according to the energy range of the known pulses, the digitizing method disclosed by the embodiment of the application can sample unknown pulses by dynamically processing the pulses or dynamically processing and setting the threshold value and combining a plurality of set threshold values, and the unknown pulses can be classified to corresponding energy addresses without fitting calculation.

Compared with the traditional MVT method, the method for digitizing the pulse signals can obtain the energy spectrum of the pulse without fitting the pulse waveform by solving the equation set to obtain the function curve in the processing process of the pulse signals, so that the process of pulse energy acquisition is simplified, more hardware resources can be saved under the condition that FPGA resources are limited, the power consumption of the FPGA is reduced, and the tolerance of the chip to high temperature is improved. The prior MVT is to collect the voltage value of the pulse through each channel, then fit the pulse waveform through sampling points, calculate the energy value of the pulse through integration, and finally draw the energy spectrum.

The conventional MVT sampling method has the advantages that the number and the size of the thresholds are fixedly set, so that the excellent effect is only suitable for the energy of a specific energy section; MVT because need fit scintillation pulse, need gather the accurate time that every point corresponds, consequently need a large amount of digital time converters (TDCs), this application embodiment through the energy way address count to scintillation pulse, reduced by a wide margin or saved the TDC for the system is succinct more, and application scope is more extensive.

In the traditional MVT method, because complex fitting calculation is required, the system cannot process new pulses within a certain period of time after each pulse is ended, and the time is dead time of the system. The embodiment of the invention bypasses the complex calculation process of pulse waveform fitting, can directly obtain energy spectrum by means of simple threshold comparison and table lookup, and greatly shortens the dead time of the work of the acquisition circuit, so that the digitizing method of the embodiment of the invention has no dead time or has very short dead time, and can basically realize continuous pulse processing.

According to some embodiments of the method and the device, the amplitude of the pulse to be detected is dynamically processed, the channel address where each pulse to be detected falls is determined, and the scheme of rapid pulse spectrum formation is realized.

Some embodiments of the present application extend the structure of the comparator chain, and the number of comparators and the number of comparison stages of each stage can be flexibly adjusted according to actual situations.

According to the method and the device, the comparison range is predetermined according to the pulse characteristics on the basis of the comparator chain, the pulse characteristics are combined with methods based on the comparator chain, such as a dichotomy method, a quartering method and the like, the pulse is divided into corresponding energy track address intervals in advance, the method and the device have advantages in application scenes of drawing high-precision energy spectrums, and spectrum forming time can be effectively shortened.

Some embodiments of the present application use a scheme of threshold time (TOT) combined with dynamic threshold spectrum formation, which is more advantageous in drawing an application scene of high-precision energy spectrum, and can effectively shorten spectrum formation time, change the sequence of voltages compared with pulses, and speed up the acquisition of comparison results as a whole.

In some embodiments of the present application, the situation that the comparators in the multi-stage comparator chain may have differences is considered, and the power spectrum can be obtained by only setting one stage of comparator by adopting a single stage comparator scheme, so that errors caused by differences between the comparators can be reduced or avoided to a certain extent.

Some embodiments of the present application further provide a step of correcting the energy track address, which further improves the accuracy of the digitizing scheme of the embodiments of the present application to draw the energy spectrum.

Accordingly, various embodiments of the present application may have at least some of the following advantages:

1) Compared with the traditional MVT method, the pulse energy spectrum can be obtained by fitting the pulse waveform without solving an equation set to obtain a function curve in the processing process of the pulse signal, the process of pulse energy acquisition is simplified, hardware resources can be greatly saved under the condition that FPGA resources are limited, the power consumption of the FPGA is reduced, and the tolerance of the chip to high temperature is improved.

2) Compared with the scheme that the ADC directly samples the pulse, the method has the advantages that the collected voltage values are not accumulated, the energy spectrum can be directly obtained, and the calculation process is simplified.

3) The traditional MVT method needs complex fitting calculation, and the system cannot process new pulses within a specific period of time after each pulse is ended, wherein the time is the dead time of the system, and the dead time is not or is very small in the digitizing scheme of the embodiment of the application, so that continuous pulse processing can be basically completed.

Accordingly, embodiments of the present application relate to a correction method 3200 for pulse digitization. As shown in fig. 32, the correction method 3200 may include steps S3210-S3280.

In the embodiment shown in fig. 32, correction method 3200 may comprise:

s3210: acquiring amplitude-energy mapping relation data of a plurality of reference pulses;

s3220: acquiring a plurality of energy addresses to be corrected, wherein each energy address to be corrected has a respective energy representation value and a corresponding determined amplitude representation value according to the amplitude-energy mapping relation data;

s3230: determining the energy addresses to be corrected corresponding to the first correction pulses according to the comparison result of the amplitude values of the first correction pulses and the amplitude characterization values of the energy addresses to be corrected;

S3240: generating an energy spectrum of the first correction pulse according to the first correction pulse count in each energy track address to be corrected and the energy characterization value of the energy track address to be corrected, wherein the energy spectrum of the first correction pulse has a first characteristic peak value;

s3250: setting a plurality of first correction energy addresses;

s3260: determining the correction energy addresses corresponding to the plurality of second correction pulses according to the comparison results of the amplitude magnitudes of the plurality of second correction pulses and the amplitude characterization values of the plurality of first correction energy addresses;

s3270: generating an energy spectrum of a second correction pulse according to the second correction pulse count in each first correction energy track address and the energy representation value of the correction energy track address, wherein the energy spectrum of the second correction pulse has a first correction characteristic peak value; and

s3280: and correcting the energy characterization values or the amplitude characterization values of the energy addresses to be corrected based on a first difference between the first characteristic peak value and the first correction characteristic peak value.

In some embodiments, the correction method may be based on a single characteristic peak.

In further embodiments, the correction method may be based on two or more characteristic peaks. Accordingly, the correction method 3200 may further include: setting a plurality of second correction energy addresses, wherein the energy ranges corresponding to the second correction energy addresses are smaller than the energy ranges corresponding to the energy addresses to be corrected, and each second correction energy address has an energy representation value and an amplitude representation value which is correspondingly determined according to the amplitude-energy mapping relation data; determining second correction energy addresses corresponding to the third correction pulses according to comparison between the amplitude values of the third correction pulses and the amplitude characterization values of the second correction energy addresses; and generating an energy spectrum of the third correction pulse according to the third correction pulse count in each second correction energy track address and the energy characterization value of the second correction energy track address, wherein the energy spectrum of the third correction pulse has a second correction characteristic peak value. Accordingly, step S3280 may include: correcting the energy characterization values or the amplitude characterization values of the plurality of energy addresses to be corrected based on a first difference between the first characteristic peak and the first correction characteristic peak and a second difference between the second characteristic peak and the second correction characteristic peak.

In embodiments of the present application, the correction method 3200 may also include steps or features of the substance constituent acquisition method, in particular sub-steps or features related to the correction steps as shown in fig. 26-29, in a non-contradictory manner, or the correction method 3200 may be combined with the substance constituent acquisition method to obtain new embodiments, or vice versa, as desired.

Furthermore, embodiments of the present application may also relate to a method of determining a composition of matter based on scintillation pulses.

In various embodiments of the present application, the scintillation pulse-based material composition determination method may employ a digitizing scheme that determines the address independently or in combination.

In some embodiments, a digitizing scheme independent of determining the addresses may be implemented, for example, in conjunction with the structure shown in fig. 20.

Referring to fig. 20 to 22, in the embodiment shown in fig. 33, the substance component determining method 3300 may include steps S3310 to S3350:

s3310: providing amplitude-energy mapping relationship data of a reference scintillation pulse generated by high-energy rays;

s3320: determining an energy window of at least one component in the substance to be detected, which corresponds to the high-energy ray;

s3330: determining a scintillation pulse amplitude range corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window;

S3340: determining the count of the scintillation pulses to be detected falling into the amplitude range according to the comparison result of the amplitude values of a plurality of scintillation pulses to be detected generated by high-energy rays emitted by the substances to be detected and the amplitude range; and

s3350: determining the content of the at least one component of the substance to be tested based on the count.

In some embodiments, there are two components.

Accordingly, in some embodiments, determining an energy window of at least one component of the substance to be measured corresponding to the high energy radiation comprises: and determining a first energy window of a first component in the substance to be detected corresponding to the high-energy ray, and determining a second energy window of a second component in the substance to be detected corresponding to the high-energy ray.

Accordingly, in some embodiments, determining the scintillation pulse amplitude range for the at least one component based on the amplitude-energy mapping data and the energy window includes: determining a first amplitude range corresponding to the first component based on the amplitude-energy mapping relationship data and the first energy window, and determining a second amplitude range corresponding to the second component based on the amplitude-energy mapping relationship data and the second energy window.

Accordingly, in some embodiments, determining a count of scintillation pulses to be measured that fall within the range of magnitudes includes: and determining a first count and a second count of scintillation pulses to be detected falling into the first amplitude range and the second amplitude range respectively. Accordingly, in some embodiments, determining the content of the at least one component of the test substance based on the count comprises: the relative amounts of the first and second ingredients are determined based on the first and second counts.

In some embodiments, the first component is carbon C and the second component is oxygen O, wherein the relative content of the first component and the second component is carbon to oxygen ratio C/O.

In the embodiment shown in fig. 34, the substance constituent determination method may be implemented in conjunction with a digitizing scheme for determining the addresses.

In the embodiment shown in fig. 34, the substance component determining method 3400 may include steps S3410 to S3460:

s3410: providing amplitude-energy mapping relationship data of a reference scintillation pulse generated by high-energy rays;

s3420: a plurality of track addresses are set up and the data is distributed,

the addresses are energy addresses or amplitude addresses, each energy address has a respective energy representation value and a corresponding amplitude representation value determined according to the amplitude-energy mapping relation data, and each amplitude address has a respective amplitude representation value;

S3430: determining the channel addresses corresponding to the scintillation pulses to be detected according to the comparison results of the amplitude values of the scintillation pulses to be detected and the amplitude characterization values of the channel addresses, wherein the scintillation pulses to be detected are generated by high-energy rays emitted by substances to be detected;

s3440: determining an energy window of at least one component in the substance to be detected, which corresponds to the high-energy ray;

s3450: determining a track address interval corresponding to the energy window based on the amplitude-energy mapping relation data and the energy window; and

s3460: and determining the content of the at least one component of the substance to be detected according to the scintillation pulse count to be detected in each channel address and the determined channel address interval.

In this embodiment, the correlated means of determining the track address described in the digitizing method of the embodiments of the present application may be utilized for determining the component content, but is not limited to whether to obtain correlated energy information or to generate an energy spectrum.

Accordingly, the material composition determining method 3400 according to the embodiment of the present application may determine the address where the scintillation pulse falls with reference to the different embodiments shown in fig. 1 to 32, which falls within the scope of the present application.

In some embodiments, referring to fig. 2-4, for example, step S3430 may include: comparing the amplitude of each scintillation pulse to be detected with comparison thresholds of a plurality of comparators in sequence, and selectively adjusting the amplitude of the scintillation pulse to be detected according to a previous comparison result before comparison, so that if the amplitude of the scintillation pulse to be detected is smaller than the comparison threshold of the previous comparator, the amplitude of the scintillation pulse to be detected is not adjusted, and if the amplitude of the scintillation pulse to be detected is larger than or equal to the comparison threshold of the previous comparator, the amplitude of the scintillation pulse to be detected is reduced, wherein the comparison thresholds of the comparators are determined according to the amplitude characterization values of a plurality of addresses; and determining the channel address corresponding to each flicker pulse to be detected according to the comparison results of the comparators.

In some embodiments, referring to fig. 5 and 6, for example, step S3430 may include: inputting each scintillation pulse to be tested into a multi-stage gate array so that the scintillation pulse to be tested sequentially passes through all stages of gates of the multi-stage gate array, wherein each gate is associated with a respective comparator and is provided with a first gate branch and a second gate branch for selectively outputting the scintillation pulse to be tested, and the gates of the non-final stage are respectively connected with two gates of the next stage through the first gate branch and the second gate branch, wherein the comparison threshold value of the comparator is determined according to the amplitude representation values of the plurality of addresses; before the scintillation pulse to be detected passes through each stage of gate, comparing the scintillation pulse to be detected with a comparator associated with the passed gate, setting the gate according to the comparison result, and determining a gate branch of the gate outputting the scintillation pulse to be detected; and determining the channel address corresponding to the flicker pulse to be detected according to the output of the multi-stage gate array.

In some embodiments, referring to fig. 7-14, for example, step S3430 may include: making the amplitude of each scintillation pulse to be tested carry out first-stage comparison of multi-stage comparison to determine the address interval in which the scintillation pulse to be tested falls, and defining at least two address intervals by at least one comparison threshold value in each stage comparison; sequentially performing next-stage comparison to determine the address interval in which the flicker pulse to be detected falls until the final-stage comparison is completed, wherein the comparison threshold value of the next-stage comparison is determined according to the address interval determined by the previous-stage comparison; and determining the address of the channel where the flicker pulse to be detected falls according to the comparison result of the last stage.

In some embodiments, for example with reference to fig. 10-13, the multi-stage comparison is implemented by a first multi-stage comparison unit comprising a plurality of parallel delay lines connected to the scintillation pulse input to be measured, an adjustable comparator connected to the delay lines, and an arbiter operatively connected to the adjustable comparator, wherein the delay times of at least some of the delay lines are different.

In some embodiments, for example with reference to fig. 10-13, the multi-stage comparison is implemented by a second multi-stage comparison unit comprising a plurality of comparator subunits connected to the scintillation pulse input to be tested and an arbiter operatively connected to the plurality of comparator subunits, wherein each comparator subunit corresponds to one of the multi-stage comparisons and comprises a single or a plurality of parallel adjustable comparators with a delay provided between adjacent comparator subunits.

In one embodiment, the comparison threshold of the first level comparison is determined from a given a priori address interval.

In some embodiments, for example, referring to fig. 23 to 24, step S3430 may include: making the amplitude of each scintillation pulse to be tested to perform a single-stage comparison comprising a plurality of comparisons to determine the address of the channel where the scintillation pulse to be tested falls, the number of the plurality of comparisons of the single-stage comparison being greater than or equal to the number of the plurality of addresses; and determining the address of the channel where the flicker pulse to be detected falls according to the comparison result of the single-stage comparison.

In some embodiments, referring to fig. 24 for example, step S3430 may include: providing threshold-crossing time-energy range mapping relationship data for a plurality of reference scintillation pulses; acquiring at least one threshold crossing time of a scintillation pulse to be detected, wherein each threshold crossing time corresponds to an amplitude threshold; determining a first address interval according to the at least one threshold crossing time and the threshold crossing time-energy range mapping relation data of the scintillation pulse to be detected; the amplitude of each scintillation pulse to be detected is subjected to single-stage comparison or multi-stage comparison to determine a second address interval in which the scintillation pulse to be detected falls, wherein each stage of comparison defines at least two second address intervals through at least one comparison threshold, and the comparison threshold of the single-stage comparison or the first stage comparison threshold of the multi-stage comparison is determined according to the first address interval; and determining the address of the flash pulse to be detected according to the single-stage or multi-stage comparison result.

In some embodiments, for example, referring to fig. 24 to 25, step S3430 may include:

providing threshold-crossing time-energy range mapping relationship data for a plurality of reference scintillation pulses; acquiring at least one threshold crossing time of a scintillation pulse to be detected, wherein each threshold crossing time corresponds to an amplitude threshold; determining a first address interval according to the at least one threshold crossing time and the threshold crossing time-energy range mapping relation data of the scintillation pulse to be detected; the amplitude of each scintillation pulse to be detected is subjected to single-stage comparison or multi-stage comparison to determine a second address interval in which the scintillation pulse to be detected falls, wherein each stage of comparison defines at least two second address intervals through at least one comparison threshold, and the comparison threshold of the single-stage comparison or the first stage comparison threshold of the multi-stage comparison is determined according to the first address interval; and determining the address of the flash pulse to be detected according to the single-stage or multi-stage comparison result.

In other embodiments, referring to fig. 25 for example, step S3430 may include: providing threshold-crossing time-energy range mapping relationship data for a plurality of reference scintillation pulses; the steps are circularly executed as follows:

setting an amplitude threshold value, obtaining the threshold-crossing time of the scintillation pulse to be detected, wherein the threshold-crossing time corresponds to the set amplitude threshold value, determining or updating a first address interval according to the threshold-crossing time of the scintillation pulse to be detected and the threshold-crossing time-energy range mapping relation data, judging whether the first address interval meets a preset standard, if yes, exiting the circulation, and if not, continuing to execute the circulation step; the amplitude of each scintillation pulse to be detected is subjected to single-stage comparison or multi-stage comparison to determine a second address interval in which the scintillation pulse to be detected falls, wherein each stage of comparison defines at least two second address intervals through at least one comparison threshold, and the comparison threshold of the single-stage comparison or the first stage comparison threshold of the multi-stage comparison is determined according to the first address interval; and determining the address of the flash pulse to be detected according to the single-stage or multi-stage comparison result.

In an embodiment of the present application, determining an energy window of at least one component in a substance to be measured corresponding to the high-energy ray includes: and determining a first energy window of a first component in the substance to be detected corresponding to the high-energy ray, and determining a second energy window of a second component in the substance to be detected corresponding to the high-energy ray.

In an embodiment of the present application, determining, based on the amplitude-energy mapping relationship data and the energy window, a track address interval corresponding to the energy window includes: and determining a first address interval corresponding to the first energy window based on the amplitude-energy mapping relation data and the first energy window, and determining a second address interval corresponding to the second energy window based on the amplitude-energy mapping relation data and the second energy window.

In an embodiment of the present application, determining the content of the at least one component of the substance to be measured according to the count of scintillation pulses to be measured in each address and the determined address range includes: determining a first count of scintillation pulses to be measured in a first address interval; determining a second count of scintillation pulses to be measured in the first address interval; and determining the relative amounts of the first and second ingredients based on the first and second counts.

In the embodiment of the application, the first component is carbon C, the second component is oxygen O, and the relative content of the first component and the second component is carbon-oxygen ratio C/O.

In embodiments of the present application, the substance component determination methods 3300, 3400 may also include steps or features of the substance component acquisition method in a non-contradictory manner as desired, particularly sub-steps or features related to the embodiments shown in fig. 20-22, or the substance component determination methods 3300, 3400 may be combined with the substance component acquisition method to obtain new embodiments, and vice versa.

Accordingly, various embodiments of the present application may provide a pulse digitizing apparatus 3500.

Fig. 35 is an exemplary block diagram of a pulse digitizing apparatus 3500 shown according to some embodiments of the application. The pulse digitizing means 3500 may comprise a mapping database 3510 comprising amplitude-energy mapping data for a plurality of reference pulses, preferably comprising an amplitude-energy look-up table for the plurality of reference pulses; an address setting unit 3520 configured to set a plurality of addresses, wherein the addresses are energy addresses or amplitude addresses, each energy address having a respective energy characterization value and a magnitude characterization value determined according to the magnitude-energy mapping relationship data, each amplitude address having a respective magnitude characterization value; a track address determining unit 3530 configured to determine track addresses corresponding to a plurality of pulses to be measured according to a comparison result of the magnitude of the plurality of pulses to be measured and the magnitude characterization value of the plurality of track addresses; and an energy information obtaining unit 3540 configured to obtain energy information of the plurality of pulses to be measured according to the pulse count to be measured in each address and the amplitude-energy mapping relationship data or the energy characterization value of the energy address.

In this embodiment, the address determining unit 3530 of the pulse digitizing apparatus 3500 may be implemented in various forms, such as features of the substance component obtaining method of the different embodiments shown with reference to fig. 1 to 31.

In some embodiments, referring to fig. 4 for example, the address determining unit 3530 may include a plurality of comparators, a plurality of gates, and a processing unit connecting the comparators and the gates, wherein the plurality of comparators are multi-stage parallel comparators, the gates are disposed between adjacent comparators, each gate includes a first gate branch and a second gate branch for selectively outputting a pulse to be measured to a lower comparator, wherein a delay is disposed in the first gate branch, and a subtractor is disposed in the second gate branch.

In some embodiments, the processing unit may be configured to receive a comparison result output by a superior comparator and set the gate according to the comparison result.

In some embodiments, the processing unit may be configured to set a reduced value of a subtractor in the gate according to the comparison result.

In some embodiments, the gate may be configured to output the pulse to be measured to the first gate branch and the second gate branch of the lower comparator according to an output level of the upper selector, and if the upper comparator output level bit is 0, output the pulse to be measured to the first gate branch of the lower comparator; and if the output level bit of the upper-stage comparator is 1, outputting the pulse to be tested to a second gating branch of the lower-stage comparator.

In some embodiments, the subtractor may be configured to reduce the amplitude of the pulse under test by a reduction value equal to a comparison threshold value of a previous comparator.

In some embodiments, referring to fig. 6 for example, the address determining unit 3530 may include a multi-stage gate array, each gate being associated with a comparator and including a first gate branch and a second gate branch for selectively outputting a pulse to be measured to a lower comparator.

In some embodiments, referring to fig. 8, 10, 12, 26 for example, the address determination unit 3530 may include a plurality of parallel delay lines coupled to the pulse input to be measured, an adjustable comparator coupled to the delay lines, and an arbiter operatively coupled to the adjustable comparator, wherein delay times of at least some of the delay lines are not identical.

In some embodiments, referring to fig. 13-17 for example, the address determination unit 3530 may include a plurality of comparator subunits coupled to the pulse input to be measured and an arbiter operatively coupled to the plurality of comparator subunits, wherein each comparator subunit corresponds to one of the multiple comparisons and includes a single or a plurality of parallel adjustable comparators, with a delay disposed between adjacent comparator subunits.

In some embodiments, the address determining unit 3530 may include a plurality of parallel adjustable comparators connected to the pulse input to be measured and an arbiter operatively connected to the plurality of parallel adjustable comparators, wherein the number of the plurality of parallel adjustable comparators is greater than, or equal to, the number of the plurality of addresses.

In embodiments of the present application, for example, referring to fig. 13-17, the arbiter may be configured to set the comparison threshold of the adjustable comparator according to the set amplitude characterizing value of the track address.

In some embodiments, referring to fig. 26 and 28 for example, the address determining unit 3530 may include a threshold-crossing time unit connected to the pulse-under-test input, a comparing unit connected to the pulse-under-test input, and an arbiter operatively connected to the threshold-crossing time unit and the comparing unit.

In some embodiments, for example with reference to fig. 26 and 28, the over-threshold time unit includes an over-threshold time comparator and an over-threshold time acquisition processor coupled to the over-threshold time comparator.

In some embodiments, the over-threshold time comparator is configured to output a transition signal when the pulse under test crosses its set amplitude threshold.

In some embodiments, the threshold-crossing time acquisition processor is configured to determine the threshold-crossing time based on a time interval between two of the transition signals from the same threshold-crossing time comparator.

In some embodiments, the arbiter is configured to determine a first address interval corresponding to the threshold crossing time from a magnitude-energy lookup table of the plurality of reference pulses.

In some embodiments, for example with reference to fig. 28, the threshold-crossing time comparators are plural, and the threshold-crossing time comparators set different magnitude thresholds to each other.

In embodiments of the present application, pulse digitizing apparatus 3500 may be used to implement substance constituent acquisition method 100 or methods described in other embodiments herein, and may optionally incorporate features of substance constituent acquisition method 100 or other methods, and vice versa.

Accordingly, various embodiments of the present application may provide a correction device 3600.

Fig. 35 is an exemplary block diagram of a correction device 3600 shown in accordance with some embodiments of the present application. The correction device 3600 may include: a first acquisition unit 3610 configured to acquire amplitude-energy mapping relationship data of a plurality of reference pulses; the second obtaining unit 3620 obtains a plurality of energy addresses to be corrected, where each energy address to be corrected has a respective energy representation value and a magnitude representation value determined according to the magnitude-energy mapping relationship data; a first address determining unit 3630 configured to determine an energy address to be corrected corresponding to a plurality of first correction pulses according to a comparison of the magnitude of the plurality of first correction pulses and the magnitude-representing value of the plurality of energy addresses to be corrected; a first energy spectrum generating unit 3640 configured to generate an energy spectrum of a first correction pulse having a first characteristic peak value according to a first correction pulse count within each energy track address to be corrected and an energy characterization value of the energy track address to be corrected; a first correction energy address setting unit 3650 configured to set a plurality of first correction energy addresses, the energy ranges corresponding to the plurality of first correction energy addresses being smaller than the energy ranges corresponding to the plurality of energy addresses, each correction energy address having a respective energy characterization value and a magnitude characterization value determined accordingly according to the magnitude-energy mapping relationship data; a second address determination unit 3660 configured to determine a correction energy address corresponding to a plurality of second correction pulses according to a comparison result of the magnitude of the plurality of second correction pulses and the magnitude characterization value of the plurality of first correction energy addresses; a second energy spectrum generating unit 3670 configured to generate an energy spectrum of a second correction pulse having a first correction characteristic peak value, based on a second correction pulse count within each first correction energy track and an energy characterization value of the correction energy track; and a correction unit 3680 configured to correct the energy or amplitude characterization values of the plurality of energy addresses to be corrected based on a first difference between the first characteristic peak and the first correction characteristic peak.

Optionally, the correction device 3600 may further include: the second correction energy address setting unit is configured to set a plurality of second correction energy addresses, the energy ranges corresponding to the plurality of second correction energy addresses are smaller than the energy ranges corresponding to the plurality of energy addresses to be corrected, and each second correction energy address has a respective energy representation value and an amplitude representation value which is correspondingly determined according to the amplitude-energy mapping relation data; a third address determination unit configured to determine second correction energy addresses corresponding to a plurality of third correction pulses according to comparison of the magnitude of the plurality of third correction pulses and magnitude characterization values of the plurality of second correction energy addresses; and a third energy spectrum generating unit for generating an energy spectrum of the third correction pulse according to the third correction pulse count in each second correction energy track address and the energy characterization value of the second correction energy track address, wherein the energy spectrum of the third correction pulse has a second correction characteristic peak value.

Optionally, the correction unit 3600 is further configured to correct an energy representation value or an amplitude representation value of the plurality of energy addresses to be corrected based on a first difference between the first characteristic peak and the first correction characteristic peak and a second difference between the second characteristic peak and the second correction characteristic peak.

In embodiments of the present application, the correction device 3600 may be used to implement the correction method 2900 or methods described in other embodiments herein, and may optionally incorporate features of the correction method 2900 or other methods, and vice versa.

Accordingly, various embodiments of the present application may provide for a substance constituent determining apparatus 3700, 3800.

As shown in fig. 37, the substance component determining apparatus 3700 may include: a mapping database 3710 comprising amplitude-energy mapping data for reference scintillation pulses generated by the high energy rays; an energy window determining unit 3720 configured to determine an energy window of at least one component of the substance to be measured corresponding to the high-energy ray; an amplitude range determining unit 3730 configured to determine a scintillation pulse amplitude range corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window; a counting unit 3740 configured to determine a count of scintillation pulses to be measured falling within the amplitude range according to a comparison result between the amplitude of the scintillation pulses to be measured generated by the high-energy rays emitted from the substance to be measured and the amplitude range; and a content determination unit 3750 configured to determine a content of the at least one component of the substance to be measured based on the count.

In some embodiments, the energy window determining unit in the substance component determining apparatus 3700 is configured to determine a first energy window in which a first component in the substance to be measured corresponds to the high energy ray and a second energy window in which a second component in the substance to be measured corresponds to the high energy ray.

In some embodiments, the amplitude range determination unit in the substance constituent determination device 3700 includes a first amplitude determination subunit and a second amplitude determination subunit configured to determine a first scintillation pulse amplitude range and a second scintillation pulse amplitude range for the first constituent, the second constituent based on the amplitude-energy mapping relationship data and the first energy window, the second energy window.

In one embodiment, the counting unit in the substance component determining apparatus 3700 further comprises: a first comparing subunit configured to determine whether the scintillation pulse to be measured falls within the first scintillation pulse amplitude range according to a comparison of the amplitude magnitude of the scintillation pulse to be measured and the first scintillation pulse amplitude range; and a second comparing subunit configured to determine whether the scintillation pulse to be measured falls within the second scintillation pulse amplitude range according to a comparison of the amplitude magnitude of the scintillation pulse to be measured and the second scintillation pulse amplitude range.

In a further embodiment, the first comparison subunit in the substance constituent determining apparatus 3700 comprises a first comparator and a second comparator, wherein the first comparator sets a comparison threshold based on a corresponding lower amplitude range limit of the first energy window, and the second comparator sets a comparison threshold based on a corresponding upper amplitude range limit of the first energy window; and the second comparing subunit includes a third comparator that sets a comparison threshold based on a corresponding lower amplitude range limit of the second energy window, and a fourth comparator that sets a comparison threshold based on an upper amplitude range limit of the second energy window.

In other embodiments, the substance constituent determining apparatus 3700 further includes a correction unit configured to obtain an operating temperature of the comparator, determine a comparison threshold deviation of the comparator at the operating temperature based on a priori information, and correct a comparison threshold of the comparator based on the comparison threshold deviation.

As shown in fig. 37, the substance component determining apparatus 3800 may include: a mapping database 3810 including amplitude-energy mapping data of reference scintillation pulses generated by the high-energy rays; an address setting unit 3820 configured to set a plurality of addresses, where the addresses are energy addresses or amplitude addresses, each energy address having a respective energy characterization value and a magnitude characterization value determined accordingly according to the magnitude-energy mapping relationship data, each amplitude address having a respective magnitude characterization value; a channel address determining unit 3830 configured to determine, according to a comparison result of the magnitude of a plurality of scintillation pulses to be measured and the magnitude characterization values of the plurality of channel addresses, channel addresses corresponding to the plurality of scintillation pulses to be measured, the plurality of scintillation pulses to be measured being generated by high-energy rays emitted by a substance to be measured; an energy window determining unit 3840 configured to determine an energy window of at least one component of the substance to be measured corresponding to the high-energy ray; a track address interval determining unit 3850 configured to determine a track address interval corresponding to the energy window based on the amplitude-energy mapping relation data and the energy window; and a content determination unit 3860 configured to determine a content of the at least one component of the substance to be measured based on the count of scintillation pulses to be measured in each of the addresses and the determined address interval.

In some embodiments, the address determining unit in the material composition determining apparatus 3800 may include a plurality of comparators, a plurality of gates, and a processing unit connected to the comparators and the gates, wherein the plurality of comparators are multistage parallel comparators, the gates are disposed between adjacent comparators, each gate includes a first gate branch and a second gate branch for selectively outputting a scintillation pulse to be measured to a lower comparator, wherein a delay is disposed in the first gate branch, and a subtractor is disposed in the second gate branch.

In some embodiments, the trace address determination unit in the material composition determining apparatus 3800 may include a plurality of parallel delay lines connected to the input of the scintillation pulse to be measured, an adjustable comparator connected to the delay lines, and an arbiter operatively connected to the adjustable comparator, wherein delay times of at least some of the delay lines are different.

In some embodiments, the address determination unit in substance constituent determination device 3800 may include a plurality of comparator subunits coupled to the input of the scintillation pulse to be measured and an arbiter operatively coupled to the plurality of comparator subunits, wherein each comparator subunit corresponds to one of the plurality of comparisons and includes a single or a plurality of parallel adjustable comparators with a delay disposed between adjacent comparator subunits.

In another embodiment, the address determination unit in substance component determination device 3800 may include a threshold-crossing time unit connected to the scintillation pulse input to be measured, a comparison unit connected to the scintillation pulse input to be measured, and an arbiter operatively connected to the threshold-crossing time unit and the comparison unit.

In embodiments of the present application, the substance constituent determining apparatus 3700, 3800 may be used to implement the substance constituent determining methods 3300, 3400 or methods described in other embodiments herein, and may optionally incorporate features of the substance constituent determining methods 3300, 3400 or other methods, or vice versa.

In the present embodiment, the pulse digitizing means 3500 may further comprise components or features of the correction means 3600 and/or the substance component determining means 3700, 3800 in a non-contradictory manner, or the pulse digitizing means 3500 may be combined with the correction means 3600 and/or the substance component determining means 3700, 3800 to obtain new embodiments, or vice versa, as desired.

It should be noted that the above description of the various steps in the figures is for illustration and description only and does not limit the application scope. Various modifications and alterations to the steps in the relevant figures may be made by those skilled in the art in light of the teachings of the present application. However, such modifications and variations are still within the scope of the present application.

It should be understood that the methods and apparatus described in the embodiments of the present application may be implemented by different systems and modules thereof. For example, in some embodiments, the system and its modules may be implemented in hardware, software, or a combination of software and hardware. Wherein the hardware portion may be implemented using dedicated logic; the software portions may then be stored in a memory and executed by a suitable instruction execution system, such as a microprocessor or special purpose design hardware. Those skilled in the art will appreciate that the methods and systems described above may be implemented using computer executable instructions and/or embodied in processor control code, such as provided on a carrier medium such as a magnetic disk, CD or DVD-ROM, a programmable memory such as read only memory (firmware), or a data carrier such as an optical or electronic signal carrier. The system and its modules of the present application may be implemented not only with hardware circuitry, such as very large scale integrated circuits or gate arrays, semiconductors such as logic chips, transistors, etc., or programmable hardware devices such as field programmable gate arrays, programmable logic devices, etc., but also with software, such as executed by various types of processors, and with a combination of the above hardware circuitry and software (e.g., firmware).

It should be noted that the above description of the modules is for convenience of description only and is not intended to limit the application to the scope of the illustrated embodiments. It will be appreciated by those skilled in the art that, given the principles of the system, various modules may be combined arbitrarily or a subsystem may be constructed in connection with other modules without departing from such principles. For example, the data acquisition module and the threshold switching module may be the same comparison module. For another example, the sampling module may also include a comparison module. For example, each module may share one memory module, or each module may have a respective memory module. Such variations are within the scope of the present application.

In some embodiments, the present application also provides a digitizing apparatus, which may include the digitizing means mentioned in the above embodiments, which may be used to collect corresponding pulse signals, such as scintillation pulse data, and generate the required energy information, such as energy power. In one specific example, the pulse digitizing apparatus provided herein may be applied to logging technology, for example, as a nuclear logging apparatus. In another specific example, the pulse digitizing apparatus provided herein may be applied to positron emission computed tomography (PET) systems where image reconstruction may be performed after gamma photon data acquisition using the scheme described in accordance with embodiments of the present application. In other specific examples of the present application, the pulse digitizing apparatus provided herein may be applied to a variety of digitizing apparatuses, such as CT apparatuses, MRI apparatuses, radiation detection apparatuses, petroleum detection apparatuses, low light detection apparatuses, SPECT apparatuses, security inspection apparatuses, gamma cameras, X-ray apparatuses, DR apparatuses, and the like, apparatuses that utilize the principle of high-energy ray conversion, and other photoelectric conversion application apparatuses, or a combination of the foregoing.

Although not shown, in some embodiments there is also provided an electronic device comprising: a memory, a processor, and an executable program stored on the memory and executable on the processor, which when executed by the processor, performs the steps of any of the methods described herein.

Although not shown, in some embodiments there is also provided a storage medium storing an executable program configured to implement steps of any of the methods described in embodiments of the present application when executed. The executable program includes respective program modules/units constituting the apparatus according to the embodiments of the present application, and the computer program constituted by the respective program modules/units is capable of realizing functions corresponding to the respective steps in the methods described in the above embodiments when executed. The executable program may also be run on an electronic device as described in embodiments of the present application.

Having described the basic concepts herein, it will be apparent to those skilled in the art that the foregoing detailed disclosure is by way of example only and is not intended to be limiting. Although not explicitly described herein, various modifications, improvements, and adaptations of the present application may occur to one skilled in the art. Such modifications, improvements, and modifications are intended to be suggested within this application, and are therefore within the spirit and scope of the exemplary embodiments of this application.

Meanwhile, the present application uses specific words to describe embodiments of the present application. Reference to "one embodiment," "an embodiment," and/or "some embodiments" means that a particular feature, structure, or characteristic is associated with at least one embodiment of the present application. Thus, it is emphasized and should be appreciated that two or more references to "an embodiment" or "one embodiment" or "an alternative embodiment" in various positions in this application are not necessarily referring to the same embodiment. Furthermore, certain features, structures, or characteristics of one or more embodiments of the present application may be combined as suitable.

Furthermore, those skilled in the art will appreciate that the various aspects of the invention are illustrated and described in the context of a number of patentable categories or circumstances, including any novel and useful procedures, machines, products, or materials, or any novel and useful modifications thereof. Accordingly, aspects of the present application may be performed entirely by hardware, entirely by software (including firmware, resident software, micro-code, etc.) or by a combination of hardware and software. The above hardware or software may be referred to as a "data block," module, "" engine, "" unit, "" component, "or" system. Furthermore, aspects of the present application may take the form of an article of manufacture in one or more readable media, comprising readable program code.

The storage medium may contain a propagated data signal with program code embodied therein, for example, on a baseband or as part of a carrier wave. The propagated signal may take on a variety of forms, including electro-magnetic, optical, etc., or any suitable combination thereof. A storage medium may be any readable medium that can communicate, propagate, or transport a program for use by or in connection with an instruction execution system, apparatus, or device. Program code located on a storage medium may be propagated through any suitable medium, including radio, cable, fiber optic cable, RF, or the like, or a combination of any of the foregoing.

Furthermore, the order in which the elements and sequences are presented, the use of numerical letters, or other designations are used in the application and are not intended to limit the order in which the processes and methods of the application are performed unless explicitly recited in the claims. While certain presently useful inventive embodiments have been discussed in the foregoing disclosure, by way of various examples, it is to be understood that such details are merely illustrative and that the appended claims are not limited to the disclosed embodiments, but, on the contrary, are intended to cover all modifications and equivalent arrangements included within the spirit and scope of the embodiments of the present application. For example, while the system components described above may be implemented by hardware devices, they may also be implemented solely by software solutions, such as installing the described system on an existing server or mobile device.

Likewise, it should be noted that in order to simplify the presentation disclosed herein and thereby aid in understanding one or more inventive embodiments, various features are sometimes grouped together in a single embodiment, figure, or description thereof. This method of disclosure, however, is not intended to imply that more features than are presented in the claims are required for the subject application. Indeed, less than all of the features of a single embodiment disclosed above.

In some embodiments, numbers describing the components, number of attributes are used, it being understood that such numbers being used in the description of embodiments are modified in some examples by the modifier "about," approximately, "or" substantially. Unless otherwise indicated, "about," "approximately," or "substantially" indicate that the number allows for a 20% variation. Accordingly, in some embodiments, numerical parameters set forth in the specification and claims are approximations that may vary depending upon the desired properties sought to be obtained by the individual embodiments. In some embodiments, the numerical parameters should take into account the specified significant digits and employ a method for preserving the general number of digits. Although the numerical ranges and parameters set forth herein are approximations that may be employed in some embodiments to confirm the breadth of the range, in particular embodiments, the setting of such numerical values is as precise as possible.

Each patent, patent application publication, and other material, such as articles, books, specifications, publications, documents, etc., cited in this application is hereby incorporated by reference in its entirety. Except for application history documents that are inconsistent or conflicting with the present application, documents that are currently or later attached to this application for which the broadest scope of the claims to the present application is limited. It is noted that the descriptions, definitions, and/or terms used in the subject matter of this application are subject to such descriptions, definitions, and/or terms if they are inconsistent or conflicting with such descriptions, definitions, and/or terms.

Finally, it should be understood that the embodiments described herein are merely illustrative of the principles of the embodiments of the present application. Other variations are also possible within the scope of this application. Thus, by way of example, and not limitation, alternative configurations of embodiments of the present application may be considered in keeping with the teachings of the present application. Accordingly, embodiments of the present application are not limited to only the embodiments explicitly described and depicted herein.

Claims

1. A substance component determining method, characterized by comprising:

determining a range of amplitude of the scintillation pulse corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window;

determining the count of the scintillation pulses to be detected falling into the amplitude range according to the comparison result of the amplitude of a plurality of scintillation pulses to be detected generated by detecting the high-energy rays emitted by the substances to be detected and the amplitude range; and

2. The method of determining a substance content according to claim 1, wherein determining an energy window of at least one component of the substance to be measured corresponding to the high-energy ray comprises:

determining a first energy window and a second energy window of a first component and a second component in the substance to be detected, which correspond to the high-energy rays respectively;

determining a scintillation pulse amplitude range corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window, comprising:

determining a first amplitude range corresponding to the first component and a second amplitude range corresponding to the second component based on the amplitude-energy mapping relation data and the first energy window and the second energy window respectively;

Determining the count of scintillation pulses to be measured falling within the amplitude range includes:

determining a first count and a second count of scintillation pulses to be detected falling into the first amplitude range and the second amplitude range respectively;

determining the content of the at least one component of the substance to be tested based on the count, comprising:

the relative amounts of the first and second ingredients are determined based on the first and second counts.

3. The substance component determining method according to claim 1 or 2, wherein the comparison of the amplitude values of the plurality of scintillation pulses to be measured with the amplitude value range is achieved by a comparator;

the substance determination method further includes:

and correcting a comparison threshold of the comparator.

4. A substance component determining method according to claim 3, wherein correcting the comparison threshold of the comparator includes:

acquiring the working temperature of a comparator;

determining a comparison threshold deviation of the comparator at the working temperature according to prior information;

and correcting the comparison threshold of the comparator according to the comparison threshold deviation.

5. A substance component determining method, characterized by comprising:

determining the channel addresses corresponding to the scintillation pulses to be detected according to the comparison results of the amplitude values of the scintillation pulses to be detected and the amplitude characterization values of the channel addresses;

6. The method according to claim 5, wherein determining an energy window of at least one component of the substance to be measured corresponding to the high-energy ray comprises:

Determining a track address interval corresponding to the energy window based on the amplitude-energy mapping relation data and the energy window, wherein the track address interval comprises the following steps:

determining a first address interval corresponding to the first energy window and a second address interval corresponding to the second energy window respectively based on the amplitude-energy mapping relation data and the first energy window and the second energy window;

determining the content of the at least one component of the substance to be measured according to the count of scintillation pulses to be measured in each address and the determined address interval, comprising: determining a first count of scintillation pulses to be measured in a first address interval;

determining a second count of scintillation pulses to be measured in the first address interval; and

7. The substance component determining method according to claim 5 or 6, wherein determining the addresses corresponding to the plurality of scintillation pulses to be measured based on a comparison result of the magnitude magnitudes of the plurality of scintillation pulses to be measured and the magnitude characterization values of the plurality of addresses, comprises:

comparing the amplitude of each scintillation pulse to be detected with comparison thresholds of a plurality of comparators in sequence, and selectively adjusting the amplitude of the scintillation pulse to be detected according to a previous comparison result before comparison;

And determining the channel address corresponding to each flicker pulse to be detected according to the comparison results of the comparators.

8. The method of claim 7, wherein selectively adjusting the amplitude of the scintillation pulse to be measured based on the previous comparison comprises:

if the amplitude of the scintillation pulse to be detected is smaller than the comparison threshold value of the previous comparator, not adjusting the amplitude of the scintillation pulse to be detected;

and if the amplitude of the scintillation pulse to be detected is greater than or equal to the comparison threshold value of the previous comparator, reducing the amplitude of the scintillation pulse to be detected, wherein the comparison threshold values of the comparators are determined according to the amplitude representation values of the plurality of addresses.

9. The substance component determining method according to claim 5, determining the addresses corresponding to the plurality of scintillation pulses to be measured based on a comparison of the magnitude of the plurality of scintillation pulses to be measured and the magnitude characterization value of the plurality of addresses, comprising:

inputting each scintillation pulse to be tested into a multi-stage gate array so that the scintillation pulse to be tested sequentially passes through all stages of gates of the multi-stage gate array, wherein each gate is associated with a respective comparator and is provided with a first gate branch and a second gate branch for selectively outputting the scintillation pulse to be tested, and the gates of the non-final stage are respectively connected with two gates of the next stage through the first gate branch and the second gate branch, wherein the comparison threshold value of the comparator is determined according to the amplitude representation values of the plurality of addresses;

Before the scintillation pulse to be detected passes through each stage of gate, comparing the scintillation pulse to be detected with a comparator associated with the passed gate, setting the gate according to the comparison result, and determining a gate branch of the gate outputting the scintillation pulse to be detected; and

and determining the channel address corresponding to the scintillation pulse to be detected according to the output of the multi-stage gate array.

10. The substance component determining method according to claim 5, determining the addresses corresponding to the plurality of scintillation pulses to be measured based on a comparison of the magnitude of the plurality of scintillation pulses to be measured and the magnitude characterization value of the plurality of addresses, comprising:

making the amplitude of each scintillation pulse to be tested carry out first-stage comparison of multi-stage comparison to determine the address interval in which the scintillation pulse to be tested falls, and defining at least two address intervals by at least one comparison threshold value in each stage comparison;

sequentially performing next-stage comparison to determine the address interval in which the flicker pulse to be detected falls until the final-stage comparison is completed, wherein the comparison threshold value of the next-stage comparison is determined according to the address interval determined by the previous-stage comparison; and

and determining the address of the channel where the flicker pulse to be detected falls according to the comparison result of the last stage.

11. The method of claim 10, wherein the multi-stage comparison is performed by a first multi-stage comparison unit comprising a plurality of parallel delay lines connected to the input of the scintillation pulse to be measured, an adjustable comparator connected to the delay lines, and an arbiter operatively connected to the adjustable comparator, wherein the delay times of at least some of the delay lines are different.

12. The method of claim 10, wherein the multi-stage comparison is performed by a second multi-stage comparison unit comprising a plurality of comparator subunits connected to the input of the scintillation pulse to be measured and an arbiter operatively connected to the plurality of comparator subunits, wherein each comparator subunit corresponds to one of the multi-stage comparisons and comprises a single or a plurality of parallel adjustable comparators, with a delay provided between adjacent comparator subunits.

13. The method of claim 10, wherein the comparison threshold of the first level comparison is determined from a given a priori address interval.

14. The substance component determining method according to claim 5, determining the addresses corresponding to the plurality of scintillation pulses to be measured based on a comparison of the magnitude of the plurality of scintillation pulses to be measured and the magnitude characterization value of the plurality of addresses, comprising:

making the amplitude of each scintillation pulse to be tested to perform a single-stage comparison comprising a plurality of comparisons to determine the address of the channel where the scintillation pulse to be tested falls, the number of the plurality of comparisons of the single-stage comparison being greater than or equal to the number of the plurality of addresses;

And determining the address of the channel where the flicker pulse to be detected falls according to the comparison result of the single-stage comparison.

15. The substance component determining method according to claim 14, wherein determining the addresses corresponding to the plurality of scintillation pulses to be measured based on a comparison result of the magnitude magnitudes of the plurality of scintillation pulses to be measured and the magnitude characterization values of the plurality of addresses, comprises:

providing threshold-crossing time-energy range mapping relationship data for a plurality of reference scintillation pulses;

acquiring at least one threshold crossing time of a scintillation pulse to be detected, wherein each threshold crossing time corresponds to an amplitude threshold;

determining a first address interval according to the at least one threshold crossing time and the threshold crossing time-energy range mapping relation data of the scintillation pulse to be detected;

the amplitude of each scintillation pulse to be detected is subjected to single-stage comparison or multi-stage comparison to determine a second address interval in which the scintillation pulse to be detected falls, wherein each stage of comparison defines at least two second address intervals through at least one comparison threshold, and the comparison threshold of the single-stage comparison or the first stage comparison threshold of the multi-stage comparison is determined according to the first address interval; and

and determining the address of the channel where the scintillation pulse to be detected falls according to the single-stage or multi-stage comparison result.

16. The substance component determining method according to claim 14, wherein determining the addresses corresponding to the plurality of scintillation pulses to be measured based on a comparison result of the magnitude magnitudes of the plurality of scintillation pulses to be measured and the magnitude characterization values of the plurality of addresses, comprises:

the steps are circularly executed as follows:

a threshold value of the amplitude value is set,

acquiring the threshold time of the scintillation pulse to be detected, wherein the threshold time corresponds to the set amplitude threshold,

determining or updating a first address interval according to the threshold crossing time and the threshold crossing time-energy range mapping relation data of the scintillation pulse to be detected,

judging whether the preset standard is met, if yes, exiting the circulation, and if not, continuing to execute the circulation step;

17. A substance component determining apparatus, characterized by comprising:

an amplitude range determining unit configured to determine an amplitude range of the scintillation pulse corresponding to the at least one component based on the amplitude-energy mapping relationship data and the energy window;

the counting unit is configured to determine the count of the scintillation pulses to be detected falling into the amplitude range according to the comparison result of the amplitude of the scintillation pulses to be detected generated by detecting the high-energy rays emitted by the substances to be detected and the amplitude range; and

18. The substance component apparatus according to claim 17, wherein the energy window determining unit is configured to determine a first energy window in which a first component in the substance to be measured corresponds to the high-energy ray and a second energy window in which a second component in the substance to be measured corresponds to the high-energy ray.

19. The substance constituent determining apparatus according to claim 17, wherein the amplitude range determining unit includes:

the first amplitude determining subunit and the second amplitude determining subunit are configured to determine a first scintillation pulse amplitude range and a second scintillation pulse amplitude range corresponding to the first component and the second component respectively based on the amplitude-energy mapping relation data and the first energy window and the second energy window.

20. The substance constituent determining apparatus according to claim 19, wherein the counting unit further comprises:

a first comparing subunit configured to determine whether the scintillation pulse to be measured falls within the first scintillation pulse amplitude range according to a comparison of the amplitude magnitude of the scintillation pulse to be measured and the first scintillation pulse amplitude range; the method comprises the steps of,

and the second comparison subunit is configured to determine whether the scintillation pulse to be detected falls into the second scintillation pulse amplitude range according to the comparison of the amplitude size of the scintillation pulse to be detected and the second scintillation pulse amplitude range.

21. The substance constituent determining apparatus according to claim 20, wherein,

the first comparison subunit comprises a first comparator and a second comparator, wherein the first comparator sets a comparison threshold value based on a corresponding lower amplitude range limit of the first energy window, and the second comparator sets a comparison threshold value based on a corresponding upper amplitude range limit of the first energy window;

The second comparison subunit includes a third comparator that sets a comparison threshold based on a corresponding lower amplitude range limit of the second energy window and a fourth comparator that sets a comparison threshold based on an upper amplitude range limit of the second energy window.

22. The substance component apparatus according to claim 19, further comprising a correction unit configured to acquire an operating temperature of a comparator, determine a comparison threshold deviation that the comparator has at the operating temperature based on a priori information, and correct a comparison threshold of the comparator based on the comparison threshold deviation.

23. A substance component determining apparatus, characterized by comprising:

The channel address determining unit is configured to determine channel addresses corresponding to the plurality of scintillation pulses to be detected according to comparison between the amplitude values of the plurality of scintillation pulses to be detected and the amplitude representation values of the plurality of channel addresses;

24. The apparatus according to claim 23, wherein the address determining unit includes a plurality of comparators, a plurality of gates, and a processing unit connecting the comparators and gates, wherein the plurality of comparators are multistage parallel comparators, the gates are provided between adjacent comparators, each gate includes a first gate branch and a second gate branch for selectively outputting a scintillation pulse to be measured to a lower comparator, wherein a delay is provided in the first gate branch, and a subtractor is provided in the second gate branch.

25. The device of claim 23, wherein the address determination unit comprises a plurality of parallel delay lines connected to the input of the scintillation pulse to be measured, an adjustable comparator connected to the delay lines, and an arbiter operatively connected to the adjustable comparator, wherein the delay times of at least some of the delay lines are different.

26. The material composition determining apparatus of claim 23, wherein the address determining unit comprises a plurality of comparator subunits connected to the input of the scintillation pulse to be measured and an arbiter operatively connected to the plurality of comparator subunits, wherein each comparator subunit corresponds to one of the plurality of comparisons and comprises a single or a plurality of parallel adjustable comparators, and a delay is provided between adjacent comparator subunits.

27. The substance constituent determining apparatus according to claim 23, wherein the address determining unit includes a threshold-crossing time unit connected to the input of the scintillation pulse to be measured, a comparing unit connected to the input of the scintillation pulse to be measured, and an arbiter operatively connected to the threshold-crossing time unit and the comparing unit.

28. An electronic device, comprising: a memory, a processor and an executable program stored on the memory and executable on the processor, which when executed by the processor, performs the steps of the substance constituent determining method according to any one of claims 1 to 16.

29. A storage medium having stored thereon an executable program which when executed by a processor performs the steps of the substance constituent determining method according to any one of claims 1 to 16.