WO2015070504A1 - 闪烁脉冲越过阈值的时间点获取方法及装置 - Google Patents
闪烁脉冲越过阈值的时间点获取方法及装置 Download PDFInfo
- Publication number
- WO2015070504A1 WO2015070504A1 PCT/CN2013/090392 CN2013090392W WO2015070504A1 WO 2015070504 A1 WO2015070504 A1 WO 2015070504A1 CN 2013090392 W CN2013090392 W CN 2013090392W WO 2015070504 A1 WO2015070504 A1 WO 2015070504A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- pulse signal
- threshold
- time
- crosses
- time point
- Prior art date
Links
- 238000000034 method Methods 0.000 title claims abstract description 35
- 230000000630 rising effect Effects 0.000 claims description 20
- 230000005540 biological transmission Effects 0.000 claims description 3
- 238000006243 chemical reaction Methods 0.000 claims description 3
- 230000009466 transformation Effects 0.000 claims 2
- 230000007704 transition Effects 0.000 description 20
- 230000004397 blinking Effects 0.000 description 13
- 235000008694 Humulus lupulus Nutrition 0.000 description 5
- 238000001514 detection method Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 239000002245 particle Substances 0.000 description 5
- 238000005070 sampling Methods 0.000 description 5
- 238000007796 conventional method Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 230000005855 radiation Effects 0.000 description 2
- 239000013078 crystal Substances 0.000 description 1
- 238000002059 diagnostic imaging Methods 0.000 description 1
- 230000009191 jumping Effects 0.000 description 1
- 238000002600 positron emission tomography Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G04—HOROLOGY
- G04F—TIME-INTERVAL MEASURING
- G04F13/00—Apparatus for measuring unknown time intervals by means not provided for in groups G04F5/00 - G04F10/00
- G04F13/02—Apparatus for measuring unknown time intervals by means not provided for in groups G04F5/00 - G04F10/00 using optical means
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03K—PULSE TECHNIQUE
- H03K5/00—Manipulating of pulses not covered by one of the other main groups of this subclass
- H03K5/01—Shaping pulses
- H03K5/08—Shaping pulses by limiting; by thresholding; by slicing, i.e. combined limiting and thresholding
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/20—Measuring radiation intensity with scintillation detectors
Definitions
- the invention relates to the fields of digital signal processing, photoelectric signal processing and radiation detection and measurement, and particularly relates to a method and a device for acquiring a time point of a scintillation pulse crossing a threshold, which can be applied to high energy particle detection and medical imaging equipment.
- scintillation detectors are often used for the detection of high-energy particles.
- the basic working principle is as follows: The high-energy particles are converted into visible light by using a scintillation crystal, and then converted into an electric pulse signal by using a photodetector. A typical electrical signal is shown in FIG. By further processing the electrical pulse, information such as energy, time, and the like of the high energy particles can be obtained.
- the time information for obtaining an electrical pulse across the threshold is widely used in the art.
- the time information of high-energy particles in the conventional method is mostly obtained by detecting the time point at which the electric pulse crosses a preset threshold.
- a multi-threshold sampling device for digitizing an electric pulse by obtaining time information of an electric pulse crossing a plurality of over-threshold points to face a conventional analog-to-digital converter (Analog to Digital Converter)
- Analog to Digital Converter Analog to Digital Converter
- the detection of the electrical pulse over the threshold time point is mostly realized by a combination of a comparator and a time-to-digital converter.
- the comparator is used to compare the relative magnitude between the electrical pulse and the threshold, and output a corresponding high and low level signal.
- the time that the pulse crosses the threshold is the high and low transition point in the comparator output signal, and the time of the trip point can be captured by the time digitizer.
- the comparator tends to output multiple high and low transitions during the period when the pulse crosses the threshold point.
- an object of the present invention is to provide a time point acquisition method and apparatus for a scintillation pulse crossing a threshold value for solving the problem that the time point due to noise cannot be accurately obtained.
- the present invention provides the following technical solutions:
- a time point acquisition method in which a scintillation pulse crosses a threshold wherein: the steps are as follows:
- the relationship between the flicker pulse and the threshold is converted into a level signal by a comparator, and the high level is output when the flicker pulse amplitude is higher than the threshold, and the output is output when the flicker pulse amplitude is lower than the threshold.
- the threshold is set, the flicker pulse signal crosses and is lower than the set threshold, the scintillation pulse signal is lower than the set threshold, the scintillation pulse signal crosses and is higher than the set threshold, and the scintillation pulse signal is higher than the set threshold, the above five stages Stage sequence occurs;
- the comparator output remains at a constant high level for the flicker pulse signal below the set threshold phase and the flicker pulse signal is above the set threshold period. Low level, no recording is performed for the time when the flicker pulse crosses the threshold.
- the flicker pulse signal is a positive pulse signal
- the scintillation pulse signal crosses and is higher than the set threshold stage. Including N time points generated by N times of hopping, the time point at which the scintillation pulse crosses the threshold is recorded as the weighted value or median value of any one of the N time points or any two or more time points of the phase.
- the phase includes M time points due to M hops, and the time point when the scintillation pulse crosses the threshold is recorded as any one of the M time points of the phase or Weighted value or median of any two or more time points; when the flicker pulse signal is a negative pulse signal, for the scintillation pulse signal crossing and lowering the threshold stage, the phase includes P times hopping At the time points of P, the time point at which the scintillation pulse crosses the threshold is recorded as the weighted value or the median value of any one of the P time points or any two or more time points in the phase, for the scintillation pulse signal to cross And above the set threshold phase, the phase includes S time points due to S times of hopping, and the time point at which the scintillation pulse crosses the threshold is recorded as S in the phase A weighted or median of any one of the time points or any two or more time points.
- the scintillation pulse signal is a positive pulse signal
- the characteristics of the five-stage level signals are respectively, and the scintillation pulse signal is low.
- the set threshold is: a low level signal; the flicker pulse signal crosses and is higher than the set threshold: the signal jumps from a low level to a high level, and follows the high and low level flips to finally become a high level;
- the flicker pulse signal is higher than the set threshold: the high level signal is continuous; the flicker pulse signal crosses and falls below the set threshold: the signal jumps from high level to low level, and follows the high and low level flips and finally becomes Low level; flicker pulse signal is lower than the set threshold: continuous low level signal; when the flicker pulse signal is negative direction pulse signal, the characteristics of the five stage level signals are respectively, the scintillation pulse signal is higher than the set threshold : Continuous high level signal;
- the flashing pulse signal crosses and falls below the set threshold: The signal jumps from high level to low level, and follows the high and low level flips and finally becomes low.
- the time point when the scintillation pulse crosses the threshold is recorded as N in the phase.
- the median point of the time point and/or at least one set of low level points that jump to a high level The weighting value, for the scintillation pulse signal crossing and lower than the set threshold period, the time point at which the scintillation pulse crosses the threshold is recorded as the median point of M time points in the phase and/or at least one set of high level jumps to low power
- the weighting value of the flat time point, when the flicker pulse signal is a negative pulse signal, for the scintillation pulse signal to cross and fall below the set threshold period, the time point when the scintillation pulse crosses the threshold is recorded as the middle of the P time points in the phase.
- a weighting value of a time point and/or a time point at which at least one set of high level jumps to a low level, for the scintillation pulse signal crossing and above a set threshold period, the time point at which the scintillation pulse crosses the threshold is recorded as S in the stage
- the median point of each time point and/or the weighted value of at least one set of low level jumps to a high level, wherein the first low level jumps to a high level and the last time
- the two time points obtained are called a group, the first time is high.
- the time point when the level jumps to the low level and the time point when the first time the high level jumps to the low level, the time point when the second high level jumps to the low level, and the second time after the last time are called a group.
- the flicker pulse signal when the flicker pulse signal is a positive pulse signal, the flicker pulse signal crosses and is higher than the set threshold period, and flickers
- the time point when the pulse crosses the threshold is recorded as the time when the first low level jumps to the high level and the time point when the first low level jumps to the high level in the stage, and the blinking pulse signal is crossed.
- the time point when the flicker pulse crosses the threshold is recorded as the time when the first high level jumps to the low level and the time when the countdown first high level jumps to the low level.
- Weighted value when the flicker pulse signal is a negative pulse signal, for the flicker pulse signal to cross and fall below the set threshold period, the time point when the flicker pulse crosses the threshold is recorded as the first high level jump to the low level in the phase.
- the time of the level and the weighting value of the time point when the first high level jumps to the low level for the first time, for the time when the scintillation pulse signal crosses and is higher than the set threshold period, the time when the scintillation pulse crosses the threshold The point is recorded as the weight of the first time the low level jumps to the high level and the time point when the first low level jumps to the high level.
- the flicker pulse signal when the flicker pulse signal is a positive pulse signal, the flicker pulse signal crosses and is higher than the set threshold period, and flickers
- the time point when the pulse crosses the threshold is recorded as the second low level jump to high power in this phase.
- the flat time and the weighted value of the time point when the second low level jumps to the high level.
- the time point when the flicker pulse crosses the threshold is recorded as the second stage of the stage.
- the weighting value, for the scintillation pulse signal crossing and higher than the set threshold period, the time point when the scintillation pulse crosses the threshold is recorded as the second low-level jump to the high level and the second lowest level in the phase. The weighted value of the time point that jumps to the high level.
- the flicker pulse signal when the flicker pulse signal is a positive pulse signal, the flicker pulse signal crosses and is higher than the set threshold period, and flickers
- the time point when the pulse crosses the threshold is recorded as weighting the N time points.
- the time point when the scintillation pulse crosses the threshold is recorded as weighting the M time points, when the flicker is obtained.
- the flashing pulse signal is crossed and lower than the set threshold period, and the time point when the blinking pulse crosses the threshold is recorded as weighting the P time points, and the blinking pulse signal is crossed and higher than the In the threshold phase, the time point at which the scintillation pulse crosses the threshold is recorded as weighting the S time points.
- the flicker pulse signal when the flicker pulse signal is a positive pulse signal, the flicker pulse signal crosses and is higher than the set threshold period, and flickers
- the time point when the pulse crosses the threshold is recorded as the median point of the N time points of the phase.
- the time point when the scintillation pulse crosses the threshold is recorded as the M time points of the phase.
- the median point, when the flicker pulse signal is a negative pulse signal, for the scintillation pulse signal crossing and lower than the set threshold phase, the time point when the scintillation pulse crosses the threshold is recorded as the median point of the P time points of the phase.
- the time point at which the scintillation pulse crosses the threshold is recorded as the median point of the S time points of the phase.
- a point in time acquisition device for a scintillation pulse crossing a threshold comprising:
- a comparing unit configured to output a level signal according to a relationship between the amplitude of the flicker pulse signal and the set threshold, output a high level when the flicker pulse amplitude is higher than the threshold, and output when the flicker pulse amplitude is lower than the threshold Low level
- the delay chain is connected by a plurality of delay units, wherein the delay unit is configured to receive and output high and low level signals;
- the scintillation pulse state time code recording unit includes a square wave signal of equal frequency, a counter, and a data buffer unit, wherein the counter is used to record the number of arrivals of the rising edge of the square wave, the data
- the buffer unit is configured to record the output signals of the delay units in the delay chain at the rising edge of the square wave signal, and the output signals of the delay chain and the arrival times of the corresponding rising edges of the square wave are combined into one time code;
- a time code classification unit for classifying an output signal of the delay chain according to the characteristics of the recorded delay chain output signal
- a relative time interpreting unit for interpreting a time interval of the hopping signal relative to a rising edge of the subsequent square wave; a time calculating and transmitting unit, calculating time information of each flipping at the time of hopping according to the time information obtained by the time interpreting unit, Selecting a point in time or weighting any two or more points in time yields an accurate point at which the scintillation pulse crosses the threshold and transmits to the next unit.
- each delay unit in the delay chain outputs the opposite value of the currently received signal state, and after the dt time, transmits the state of the previous time to the next one.
- the cascaded delay unit simultaneously accepts the signal transmitted by the delay unit of the previous cascade and outputs the opposite value of the state.
- the frequency range of the square wave signal of the medium frequency of the scintillation pulse state time code recording unit is 20 GHz to 10 MHz.
- the output signals of the delay chain in the time code classification unit are classified into five categories, and for a forward scintillation pulse, the scintillation pulse signal is specifically divided into lower
- the threshold is set, the scintillation pulse signal is crossed and is higher than the set threshold, the scintillation pulse signal is higher than the set threshold, the scintillation pulse signal is crossed and lower than the set threshold, and the scintillation pulse signal is lower than the set threshold
- the above five stages Sequence occurs, for a negative blinking pulse, specifically divided into a flicker pulse signal higher than the set threshold, the scintillation pulse signal is crossed and below the set threshold, the scintillation pulse signal is lower than the set threshold, and the scintillation pulse signal is crossed and higher than
- the set threshold and the flicker pulse signal are higher than the set threshold five stages, and the above five stages occur sequentially.
- each The characteristic of the class is that the flicker pulse signal is lower than the set threshold: all are continuous T; the flicker pulse signal crosses and is higher than the set threshold: the output signal from the low effective bit to the high effective bit is a plurality of consecutive '0, after Convert to T and follow '0' multiple times, T transform is a number of consecutive T; flicker pulse signal is higher than the set threshold: all are continuous '0,; the flicker pulse signal crosses and is lower than the set threshold: output The signal is converted from a low-significant bit to a high-significant bit to a plurality of consecutive Ts, and is followed by a number of ⁇ , '0, and converted to a plurality of consecutive '0'; the scintillation pulse signal is below the set threshold: All are continuous ⁇ ; When the flicker pulse signal is a negative pulse signal, each type is characterized by a flicker pulse signal higher than the set threshold: all are continuous '0,; the flicker pulse signal
- the relative time interpreting unit when the scintillation pulse signal crosses and is higher than the set threshold state, From the low to the high position, the number of delay units in the first occurrence of ⁇ is used to characterize the time when the first low level jumps to the high level. From the low order to the high level, the last occurrence of '0, the time delay unit The number of times is used to represent the time when the last low level jumps to the high level; when the blinking pulse signal crosses and is lower than the set threshold state, the number of delay units when the last occurrence of ⁇ occurs from the low to the high level.
- the flicker pulse signal is a negative pulse signal
- the relative time interpreting unit when the flicker pulse signal crosses and is lower than the set threshold state, the first occurrence from the low bit to the high bit counts' 0, the number of time delay units is used to characterize the time when the first high level jumps to the low level. From the low order to the high level, the number of delay units in the last occurrence of the ⁇ is used to represent the last high power.
- the time to jump to the low level; when the flicker pulse signal crosses and is higher than the set threshold, the last occurrence of '0 from the low to the high level is used to characterize the first low power.
- the time to jump to the high level the number of delay units from the low to the high level is the first time the ⁇ is used to represent the last low power. The time to jump to the high level.
- the time point acquisition method and apparatus for the scintillation pulse of the present invention exceeds the threshold by using the obtained time of the multiple transition edges by selecting one transition time point or for any two or more transitions.
- the time point is weighted to obtain a more accurate time at which the pulse actually crosses the threshold, in particular by obtaining the time when the scintillation pulse crosses the first hop and the last hop in the threshold phase, by weighting the two times, More accurately obtaining the time point at which the scintillation pulse actually crosses the threshold, the present invention also finds the first hop by searching for the output of the delay chain looking for '0-1, or '1-0, the position of the hopping and the relationship between them.
- FIG. 1 is a schematic diagram of a typical scintillation pulse waveform in the prior art
- FIG. 2 is a schematic diagram of another scintillation pulse waveform in the prior art
- FIG. 3 is a schematic diagram showing a state in which the logic output signal formed by the scintillation pulse in FIG. 2 passes through the comparator and the corresponding delay chain output signal from the low significant bit (LSB) to the high significant bit (MSB);
- FIG. 4 is a schematic diagram of time sampling points at four different thresholds obtained by a time point acquisition method in which the scintillation pulse of the present invention crosses a threshold.
- DETAILED DESCRIPTION OF THE INVENTION The present invention discloses a method and apparatus for acquiring a time point at which a scintillation pulse crosses a threshold value, which is used to solve the problem that the time point due to noise cannot be accurately obtained.
- the flicker pulse signal can be a positive pulse signal or a negative pulse signal
- the present invention describes both positive and negative pulses.
- the method for acquiring a time point at which a scintillation pulse of the present invention crosses a threshold is as follows:
- the relationship between the flicker pulse and the threshold is converted into a level signal by a comparator, and the high level is output when the flicker pulse amplitude is higher than the threshold, and the output is output when the flicker pulse amplitude is lower than the threshold. level.
- the threshold is set, the flicker pulse signal crosses and is lower than the set threshold, the scintillation pulse signal is lower than the set threshold, the scintillation pulse signal crosses and is higher than the set threshold, and the scintillation pulse signal is higher than the set threshold, the above five stages The sequence of phases takes place.
- the flicker pulse signal when the flicker pulse signal is a positive pulse signal, the characteristics of the five-stage level signals are respectively, the flicker pulse signal is lower than the set threshold: the low level signal is continued; the flicker pulse signal crosses and is higher than the set threshold : The signal jumps from low level to high level, and follows the high and low level flips and finally turns to high level; the flicker pulse signal is higher than the set threshold: continuous high level signal; flicker pulse signal crossing and low Set the threshold: The signal jumps from high level to low level, and follows the high and low level flips and finally turns to low level; the flicker pulse signal is lower than the set threshold: continuous low level signal.
- the flicker pulse signal when the flicker pulse signal is a negative pulse signal, the characteristics of the five-stage level signals are respectively, the flicker pulse signal is higher than the set threshold: the high level signal is continued; the flicker pulse signal crosses and is lower than the set threshold : The signal jumps from high level to low level, and follows the high and low level flips and finally turns to low level; the flicker pulse signal is lower than the set threshold: continuous low level signal; flicker pulse signal crossing and high Set the threshold: The signal jumps from low level to high level, and follows the high and low level flips and finally turns to high level; the flicker pulse signal is higher than the set threshold: Continuous high level signal.
- the scintillation pulse signal is low.
- the comparator output maintains a constant level (either high level or low level), and the time in both cases is generally not recorded.
- the pulse signal crosses the threshold phase and triggers the comparator to generate a high-low level flip, the time is recorded, so the time point when the flicker pulse in these two phases crosses the threshold is not recorded.
- the phase When the flicker pulse signal is a positive pulse signal, for the flicker pulse signal to cross and exceed the set threshold phase, the phase includes N time points due to N times of hopping, and the time point at which the scintillation pulse crosses the threshold is recorded as A weighting value or a median value of any one of the N time points or any two or more time points of the phase, for the scintillation pulse signal crossing and lower than the set threshold phase, the phase including the M hopping M time points, the time point at which the flicker pulse crosses the threshold is recorded as the weighted value or median value of any one of the M time points or any two or more time points in the phase; when the flicker pulse signal is negative For the pulse signal, for the scintillation pulse signal crossing and lowering the threshold period, the phase includes P time points due to P times of hopping, and the time point when the scintillation pulse crosses the threshold is recorded as P time points in the phase.
- the weighted value or median of any one time point or any two or more time points, for the scintillation pulse signal to cross and exceed the set threshold Segment, this phase includes S time points due to S times of hopping, and the time point at which the scintillation pulse crosses the threshold is recorded as any one of the S time points in the phase or any two or more time points. Weighted or median.
- the present invention can arbitrarily select some of the time points after the time point of the N (M, P, S) hopping (may be one of the points, or
- the two points can also be n points, which can be continuous or non-continuous, can be extracted regularly or irregularly, or all time points can be weighted or taken.
- the median point to represent the exact point in time.
- the further superior protection range of the invention with respect to the step (3) is: when the scintillation pulse signal is a positive pulse signal, the time point at which the scintillation pulse crosses the threshold is recorded as the median point of the N time points in the phase and/or a weighting value of at least one set of low-level jumps to a high level, for the scintillation pulse signal crossing and lower than the set threshold period, the time point at which the scintillation pulse crosses the threshold is recorded as the middle of the M time points in the phase a weighted value of a point in time and/or at least one set of high level jumps to a low level, when the flicker pulse signal is a negative pulse signal, the flicker pulse signal is crossed and is lower than the set threshold step Segment, the time point at which the scintillation pulse crosses the threshold is recorded as the weighted value of the median point of the P time points of the phase and/or the time point of at least one set of the high level jumping to the low level, for the scint
- the time point when the first low level jumps to the high level and the time point when the first low level jumps to the high level, and the time point when the second low level jumps to the high level And the time point when the penultimate low level jumps to the high level and the two time points obtained by the analogy are called a group
- a time point when a second high level jumps to a low level a time point when a second high level jumps to a low level
- the two time points obtained by analogy are called a group.
- the first further superior protection range of the invention with respect to the step (3) is: when the scintillation pulse signal is a positive pulse signal, the time for the scintillation pulse to cross the threshold for the scintillation pulse signal crossing and above the set threshold phase
- the point record is the weighted value of the time when the first low level jumps to the high level and the time point when the first low level jumps to the high level in the stage, and the flashing pulse signal is crossed and lower than the set value.
- the threshold phase the time point at which the flicker pulse crosses the threshold is recorded as the weighted value of the time when the first high level jumps to the low level and the time point when the countdown first high level jumps to the low level.
- the time point when the flicker pulse crosses the threshold is recorded as the time when the first high level jumps to the low level in the stage.
- the weighting value of the time point when the first high level jumps to the low level, and the flashing pulse signal crosses and is higher than the set threshold period, and the time point when the blinking pulse crosses the threshold is recorded as the stage.
- the second further superior protection range of the present invention with respect to the step (3) is: when the scintillation pulse signal is a positive pulse signal, the time when the scintillation pulse signal crosses the threshold for the scintillation pulse signal crossing and above the set threshold period
- the point record is the weighted value of the time when the second low level jumps to the high level at this stage and the time point when the second low level jumps to the high level, and the flashing pulse signal is crossed and lower than the set value.
- the time point at which the blinking pulse crosses the threshold is recorded as the weighted value of the time when the second high level jumps to the low level and the time point when the second last high level jumps to the low level.
- the flashing pulse signal crosses and is lower than the set threshold period, flashing
- the time point when the blinking pulse crosses the threshold is recorded as the weighting value of the time when the second high level jumps to the low level and the time point when the second highest level jumps to the low level, for the blinking pulse signal.
- the time point when the flicker pulse crosses the threshold is recorded as the time when the second low level jumps to the high level and the time when the second last low level jumps to the high level. The weight of the point.
- the third further superior protection range of the present invention with respect to the step (3) is: when the scintillation pulse signal is a positive pulse signal, the time when the scintillation pulse signal crosses the threshold for the scintillation pulse signal crossing and above the set threshold period The point record is obtained by weighting the N time points. For the scintillation pulse signal to cross and lower than the set threshold period, the time point when the scintillation pulse crosses the threshold is recorded as weighting the M time points, and the scintillation pulse signal is negative.
- the time point when the flicker pulse crosses the threshold is recorded as weighting the P time points, and the flicker pulse signal is crossed and higher than the set threshold period, and flickering The point in time when the pulse crosses the threshold is recorded as weighting the S time points.
- the fourth further superior protection range of the present invention with respect to the step (3) is: when the scintillation pulse signal is a positive pulse signal, the time when the scintillation pulse signal crosses the threshold for the scintillation pulse signal crossing and above the set threshold phase The point is recorded as the median point of the N time points of the phase. For the scintillation pulse signal to cross and fall below the set threshold phase, the time point at which the scintillation pulse crosses the threshold is recorded as the median point of the M time points of the phase.
- the time point at which the scintillation pulse crosses the threshold is recorded as the median point of the P time points of the phase, and the scintillation pulse signal is crossed. And above the set threshold phase, the time point at which the scintillation pulse crosses the threshold is recorded as the median point of the S time points of the phase.
- the time point at which the blinking pulse actually crosses the threshold can be obtained not only by the weighting of the first hopping and the last hopping time, but also by the second and the second last. Sub-weighted (and so on).
- the median point can also be used, or even by the method of likelihood estimation.
- the invention mainly finds the time of the first hop, the last hop and even all the middle hops by analyzing the output of the delay chain to find ' ⁇ - ⁇ or '1-0, the position of the hopping and the relationship between them. Obtain.
- the present invention also discloses a time point acquisition device for a scintillation pulse crossing a threshold, comprising: a comparison unit, a delay chain, a scintillation pulse state time code recording unit, a time code classification unit, a relative time interpretation unit, and a time calculation and transmission unit.
- the comparing unit is configured to output a level signal according to a relationship between the amplitude of the flicker pulse signal and the set threshold, output a high level when the flicker pulse amplitude is higher than the threshold, and output a low level when the flicker pulse amplitude is lower than the threshold.
- the delay chain is formed by concatenating a plurality of delay units for accepting and outputting high and low level signals.
- Each delay unit in the delay chain outputs the opposite value of the currently accepted signal state, and after the dt time, transmits the state of the previous time to the next cascaded delay unit, and accepts the previous cascaded delay unit. The signal transmitted to and outputs the opposite value of the state.
- the flicker pulse state time code recording unit includes a square wave signal of equal frequency, a counter and a data buffer unit, wherein the counter is used to record the number of arrivals of the rising edge of the square wave, and the data buffer unit is configured to record the square wave signal.
- the output signal of each delay unit in the delay chain at the rising edge time, the output signal of the delay chain and the number of arrivals of the corresponding rising edge of the square wave are combined into one time code.
- the frequency range of the equal-frequency square wave signal is 20 GHz to 10 MHz.
- the counter is used to record the number of arrivals of the rising edge of the square wave
- the data buffer unit is configured to record the output signals of the delay units in the delay chain at the rising edge of the square wave signal, the output signal of the delay chain and the corresponding The number of arrivals of the rising edge of the square wave is combined into one time code.
- the time code classification unit is configured to classify the output signal of the delay chain according to the characteristics of the recorded delay chain output signal.
- the output signals of the delay chain in the time code classification unit are classified into five types.
- a forward flicker pulse the scintillation pulse signal is specifically lower than the set threshold, the scintillation pulse signal is crossed and higher than the set threshold, and the scintillation pulse is The signal is above the set threshold, the scintillation pulse signal is crossed and below The set threshold and the flicker pulse signal are lower than the set threshold.
- the above five stages occur sequentially.
- For a negative flicker pulse the scintillation pulse signal is higher than the set threshold, and the scintillation pulse signal is crossed and lower.
- the above five stages are sequentially generated in the five stages of setting the threshold, the flicker pulse signal is lower than the set threshold, the scintillation pulse signal is crossed and higher than the set threshold, and the scintillation pulse signal is higher than the set threshold.
- each type of characteristic is that the flicker pulse signal is lower than the set threshold: all are continuous T; the flicker pulse signal crosses and is higher than the set threshold: the output signal is low effective bit
- the high effective bit is a plurality of consecutive '0's, then converted to T and followed by multiple '0', and the T transform is a plurality of consecutive T; the scintillation pulse signal is higher than the set threshold: all are consecutive '0, ;
- the flicker pulse signal crosses and falls below the set threshold: The output signal is from continuous low to high active bit for multiple consecutive
- each type is characterized by a flicker pulse signal higher than the set threshold: all are continuous '0,; the flicker pulse signal crosses and falls below the set threshold: the output signal is low
- the valid bit to the high significant bit is converted to '0 after multiple consecutive turns, and is followed by multiple ⁇ , '0, after conversion is a plurality of consecutive '0'; the flicker pulse signal is lower than the set threshold: all are continuous
- the flashing pulse signal crosses and is above the set threshold: the output signal is from continuous low to high active.
- ⁇ transform is a number of consecutive ⁇ ; flicker pulse signal is higher than the set threshold: all are consecutive '0'.
- the relative time interpretation unit is configured to interpret the time interval of the hopping signal relative to the rising edge of the subsequent square wave.
- the flicker pulse signal is a forward pulse signal
- the first time delay time unit of the ⁇ time period is counted from the low bit to the high bit
- the number is used to characterize the time when the first low level jumps to the high level. From the low to the high level, the last occurrence of '0, the number of delay units is used to represent the last low level jump to high power.
- Flat time in the state where the flicker pulse signal crosses and is lower than the set threshold, the number of delay units from the low bit to the high bit count last time is used to characterize the first high level jump to the low level.
- Time from the low to the high level, the first occurrence of '0, the number of delay units is used to represent the time when the last high level jumped to low level.
- the flicker pulse signal is a negative pulse signal
- the first time occurrence of '0 the time delay unit from the low bit to the high bit count
- the number of times is used to characterize the time when the first high level jumps to the low level. From the low order to the high level, the number of delay units when the last occurrence of T is used to represent the last high level jump to low power.
- the time calculation and the transmission unit calculate the time information of each flip when the hop occurs according to the time information obtained by the time interpretation unit, and obtain an accurate time by selecting a time point or weighting any two or more time points.
- the flashing pulse crosses the threshold time point and is transmitted to the next unit.
- FIG. 3 is a schematic diagram showing a state in which a logic output signal formed when a scintillation pulse passes through a comparator and a corresponding delay chain output signal from a low significant bit (LSB) to a high significant bit (MSB).
- LSB low significant bit
- MSB high significant bit
- time information when the scintillation pulse crosses the reference threshold voltage is captured. Since the rising edge of the pulse is not affected by noise, the logic signal is stably maintained in a high state after only one transition occurs when the pulse crosses and exceeds the threshold; the falling edge of the pulse is partially affected by noise when the pulse crosses and falls below the threshold. When a transition occurs, it is stabilized in a logic low state after a number of state changes.
- A, B, and C respectively represent the upper edge of the pulse crossing and above the threshold phase; the pulse crosses and falls below the first lower edge and the last lower edge of the threshold phase.
- the logic signal is input into the delay chain.
- the output of the delay chain under the rising edge of different clocks is shown on the left side of the figure.
- three delay chains are used in this example to record the time when A, B, and C occur, and three delay chains use three different coding modes.
- the delay chain used is composed of m adder cascades, the addend of each stage adder is set to 1, and all addends are set to 0, when connected to the carry-in chain of the first stage adder of the carry chain
- the adder output Sum will transition from high to low, as indicated by point A in Figure 3.
- the carry chain is composed of m adder cascades, the addend of each adder is set to 1, and all addends are set to 0, when connected to the comparator output of the carry stage of the first stage adder of the carry chain
- the adder output Sum will transition from high to low, as indicated by point B in Figure 3, by encoding into the delay chain from the high (MSB) to the low ( LSB)
- N The number N of consecutive occurrences. If the delay of each adder is T, then N*T is the time interval between the time of B and the rising edge of the current clock.
- the carry chain is composed of m adder cascades, the addend of each adder is set to 1, and all addends are set to 0.
- the adder output Sum will transition from high to low, as indicated by point C in Figure 3, by encoding into the delay chain from the low (LSB) to the high ( MSB) The number N of consecutive occurrences. If the delay of each adder is T, then (mN) *T is the time interval between the C time and the rising edge of the current clock.
- the time interval obtained by the above method, and the time of three times A, B, and C can be obtained according to the number of clock cycles recorded by the time counter.
- the time sampling points at different thresholds obtained by the method are given in FIG. 4 (the results of four different thresholds are given in FIG. 4, that is, the acquisition of the time using points under each threshold is adopted in the present invention.
- the method described where the dot is the actual acquired sample point.
- the time at which the scintillation pulse actually crosses the threshold is obtained by weighting the two sample points obtained by the falling edge portion of the scintillation pulse, that is, the point marked by the asterisk in the figure.
- the present invention provides a method for solving the problem of inaccurate sampling of voltage time due to noise.
- the conventional method does not consider the noise of the falling edge portion of the scintillation pulse, and directly adopts the first transition edge as the time point at which the pulse crosses the threshold. In this way, in the case of noise, the collected time must be earlier than the time when the pulse actually crosses the threshold, and the acquisition accuracy is insufficient.
- the invention proposes a time acquisition method for realizing all the transition edges of the pulse crossing the threshold phase
- the invention obtains these time points mainly by studying the output state on the carry chain. To the point in time of each jump.
- the present invention achieves the time to acquire the first edge and the last edge. Take advantage of the two points obtained.
- the time point acquisition method and apparatus for the scintillation pulse of the present invention crossing the threshold value obtains a more accurate pulse by using the obtained time of the plurality of transition edges by the median point and/or at least one set of hopping along the time to obtain a more accurate pulse.
- the point in time of the threshold is obtained by using the obtained time of the plurality of transition edges by the median point and/or at least one set of hopping along the time to obtain a more accurate pulse.
- the present invention finds '0-1, or '1-0, the position of the hopping and the relationship between them by analyzing the output of the delay chain to realize the time acquisition of the first hop, the last hop, and even all the intermediate hops. .
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Measurement Of Radiation (AREA)
- Nuclear Medicine (AREA)
Abstract
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2016529452A JP6251393B2 (ja) | 2013-11-14 | 2013-12-25 | 微光パルスがしきい値を通過した時点を取得するための方法およびデバイス |
EP13897366.4A EP3070847B1 (en) | 2013-11-14 | 2013-12-25 | Method and device for acquiring time point where glimmering pulse passes over threshold |
US15/035,996 US10120342B2 (en) | 2013-11-14 | 2013-12-25 | Method and device for acquiring time point where glimmering pulse passes over threshold |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310572921.0 | 2013-11-14 | ||
CN201310572921.0A CN104639123B (zh) | 2013-11-14 | 2013-11-14 | 闪烁脉冲越过阈值的时间点获取方法及装置 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2015070504A1 true WO2015070504A1 (zh) | 2015-05-21 |
Family
ID=53056675
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/CN2013/090392 WO2015070504A1 (zh) | 2013-11-14 | 2013-12-25 | 闪烁脉冲越过阈值的时间点获取方法及装置 |
Country Status (6)
Country | Link |
---|---|
US (1) | US10120342B2 (zh) |
EP (1) | EP3070847B1 (zh) |
JP (1) | JP6251393B2 (zh) |
CN (1) | CN104639123B (zh) |
HU (1) | HUE042347T2 (zh) |
WO (1) | WO2015070504A1 (zh) |
Families Citing this family (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105842544B (zh) * | 2016-03-18 | 2018-09-18 | 南京瑞派宁信息科技有限公司 | 一种迭代的闪烁脉冲时间标记及其交叉验证方法 |
WO2020035937A1 (ja) * | 2018-08-17 | 2020-02-20 | 三菱電機株式会社 | 放射線計測装置 |
CN109171787B (zh) * | 2018-08-27 | 2021-02-26 | 苏州瑞派宁科技有限公司 | 脉冲信号的采样方法、装置和计算机程序介质 |
CN110061733B (zh) * | 2019-04-19 | 2023-04-04 | 苏州瑞迈斯医疗科技有限公司 | 脉冲信号的计数方法、重建方法及芯片 |
CN111158039B (zh) * | 2020-01-02 | 2022-01-04 | 苏州瑞派宁科技有限公司 | 信号采样、重建方法及装置 |
CN115032877B (zh) * | 2022-05-26 | 2024-03-29 | 合肥综合性国家科学中心人工智能研究院(安徽省人工智能实验室) | 脉冲的采样方法、采样系统、装置及计算机可读存储介质 |
CN115113512B (zh) * | 2022-05-26 | 2024-03-29 | 合肥综合性国家科学中心人工智能研究院(安徽省人工智能实验室) | 脉冲的采样方法、采样系统、装置及计算机可读存储介质 |
CN118473552B (zh) * | 2024-07-09 | 2024-10-11 | 深圳市华茂欧特科技有限公司 | 通信系统的数据传输时长测量方法、装置、设备及介质 |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1303174A (zh) * | 1999-12-10 | 2001-07-11 | 吕跃进 | 内烁脉冲器及用途 |
CN102262238A (zh) * | 2011-04-19 | 2011-11-30 | 苏州瑞派宁科技有限公司 | 一种提取闪烁脉冲信息的方法及装置 |
CN202177701U (zh) * | 2011-04-19 | 2012-03-28 | 苏州瑞派宁科技有限公司 | 一种提取闪烁脉冲信息的装置 |
CN102843139A (zh) * | 2012-09-20 | 2012-12-26 | 苏州瑞派宁科技有限公司 | 一种闪烁脉冲数字化的方法及装置 |
CN202801645U (zh) * | 2012-09-20 | 2013-03-20 | 苏州瑞派宁科技有限公司 | 一种闪烁脉冲数字化的装置 |
Family Cites Families (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5148178A (en) * | 1988-10-11 | 1992-09-15 | Santa Barbara Research Center | Precision ranging system |
US7617270B2 (en) * | 2002-10-07 | 2009-11-10 | Nikitin Alexei V | Method and apparatus for adaptive real-time signal conditioning, processing, analysis, quantification, comparison, and control |
JP4279798B2 (ja) * | 2004-04-02 | 2009-06-17 | 財團法人国家衛生研究院 | アナログ/デジタル変換器を使用せず、ガンマ線エネルギーをデジタル化し、ピーク期間と減衰期間の時間定数を特徴付けする装置及び使用法 |
GB2421317B (en) * | 2004-12-15 | 2009-02-11 | Agilent Technologies Inc | A method and apparatus for detecting leading pulse edges |
CN101600972B (zh) | 2006-07-28 | 2012-08-29 | 皇家飞利浦电子股份有限公司 | 正电子发射断层摄影中的飞行时间测量 |
JP5161444B2 (ja) * | 2006-08-11 | 2013-03-13 | テクトロニクス・インコーポレイテッド | ジッタ特性分析プログラム及びジッタ特性の表又はグラフ表示方法 |
GB2441572B (en) | 2006-09-05 | 2009-01-28 | Stream Technology Ltd M | Switching amplifier |
US8598536B2 (en) | 2006-10-04 | 2013-12-03 | CERN—European Organization for Nuclear Research | Apparatus and method for medical imaging |
JP2008092387A (ja) * | 2006-10-04 | 2008-04-17 | Nagasaki Univ | アナログ・デジタル変換回路、タイミング信号発生回路および制御装置 |
JP4585545B2 (ja) | 2007-06-29 | 2010-11-24 | 株式会社豊田中央研究所 | ノイズ除去回路及びそれを備えたコンパレータ回路 |
US8258480B2 (en) * | 2008-03-03 | 2012-09-04 | The Board Of Trustees Of The Leland Stanford Junior University | High energy photon detection using pulse width modulation |
-
2013
- 2013-11-14 CN CN201310572921.0A patent/CN104639123B/zh active Active
- 2013-12-25 JP JP2016529452A patent/JP6251393B2/ja active Active
- 2013-12-25 HU HUE13897366A patent/HUE042347T2/hu unknown
- 2013-12-25 US US15/035,996 patent/US10120342B2/en active Active
- 2013-12-25 WO PCT/CN2013/090392 patent/WO2015070504A1/zh active Application Filing
- 2013-12-25 EP EP13897366.4A patent/EP3070847B1/en active Active
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1303174A (zh) * | 1999-12-10 | 2001-07-11 | 吕跃进 | 内烁脉冲器及用途 |
CN102262238A (zh) * | 2011-04-19 | 2011-11-30 | 苏州瑞派宁科技有限公司 | 一种提取闪烁脉冲信息的方法及装置 |
CN202177701U (zh) * | 2011-04-19 | 2012-03-28 | 苏州瑞派宁科技有限公司 | 一种提取闪烁脉冲信息的装置 |
CN102843139A (zh) * | 2012-09-20 | 2012-12-26 | 苏州瑞派宁科技有限公司 | 一种闪烁脉冲数字化的方法及装置 |
CN202801645U (zh) * | 2012-09-20 | 2013-03-20 | 苏州瑞派宁科技有限公司 | 一种闪烁脉冲数字化的装置 |
Also Published As
Publication number | Publication date |
---|---|
JP6251393B2 (ja) | 2017-12-20 |
US10120342B2 (en) | 2018-11-06 |
EP3070847B1 (en) | 2018-12-19 |
US20160274547A1 (en) | 2016-09-22 |
EP3070847A1 (en) | 2016-09-21 |
CN104639123B (zh) | 2017-08-25 |
JP2017501387A (ja) | 2017-01-12 |
CN104639123A (zh) | 2015-05-20 |
EP3070847A4 (en) | 2017-08-02 |
HUE042347T2 (hu) | 2019-06-28 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
WO2015070504A1 (zh) | 闪烁脉冲越过阈值的时间点获取方法及装置 | |
US8970421B1 (en) | High resolution sampling-based time to digital converter | |
US7345604B2 (en) | Analog to digital conversion using recurrent neural networks | |
Wang et al. | A 3.0-ps rms precision 277-MSamples/s throughput time-to-digital converter using multi-edge encoding scheme in a Kintex-7 FPGA | |
CN109274369B (zh) | 一种闪烁脉冲数字化的方法及装置 | |
CN109936360B (zh) | 脉冲计数装置及辐射探测系统 | |
US6492929B1 (en) | Analogue to digital converter and method of analogue to digital conversion with non-uniform sampling | |
WO2012088781A1 (zh) | 一种数字化pileup波形处理方法及系统 | |
JP6336070B2 (ja) | シンチレーションパルス情報を回復するための方法およびシステム | |
WO2014121530A1 (zh) | 一种多阈值采样数字化器件的阈值校正方法 | |
US7876873B2 (en) | Asynchronous ping-pong counter and thereof method | |
JP5666813B2 (ja) | 時間幅測定装置 | |
KR20150127928A (ko) | 카운터, 그 카운터를 포함하는 아날로그/디지털 컨버터 및 그 아날로그/디지털 컨버터를 포함하는 이미지 센싱 장치 | |
CN110061733B (zh) | 脉冲信号的计数方法、重建方法及芯片 | |
CN108964663A (zh) | 一种基于预测算法的心电信号特征参数提取方法 | |
CN110988961B (zh) | 信号处理方法、装置和探测系统 | |
US20170222655A1 (en) | Analog-to-digital converter, electronic device, and method of controlling analog-to-digital converter | |
KR101463062B1 (ko) | 신호 처리 장치 및 방법, 그를 이용한 수신기 그리고 거리 측정 장치 | |
CN106712776A (zh) | 连续渐近式类比数位转换器及其控制方法 | |
Delagnes | What is the theoretical time precision achievable using a dCFD algorithm? | |
CN104749407B (zh) | 示波器触发脉宽检测方法、装置及一种示波器 | |
CN107241101B (zh) | 数据串行化电路 | |
TWI282860B (en) | Apparatus and method for time-to-digital conversion and jitter measuring apparatus and method using the same | |
CN116412906A (zh) | 单光子多脉冲探测方法、系统及功能电路 | |
CN115113512B (zh) | 脉冲的采样方法、采样系统、装置及计算机可读存储介质 |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
121 | Ep: the epo has been informed by wipo that ep was designated in this application |
Ref document number: 13897366 Country of ref document: EP Kind code of ref document: A1 |
|
ENP | Entry into the national phase |
Ref document number: 2016529452 Country of ref document: JP Kind code of ref document: A |
|
WWE | Wipo information: entry into national phase |
Ref document number: 15035996 Country of ref document: US |
|
NENP | Non-entry into the national phase |
Ref country code: DE |
|
REEP | Request for entry into the european phase |
Ref document number: 2013897366 Country of ref document: EP |
|
WWE | Wipo information: entry into national phase |
Ref document number: 2013897366 Country of ref document: EP |