CN102058938B - Imaging system for ionizing radiation - Google Patents

Imaging system for ionizing radiation Download PDF

Info

Publication number
CN102058938B
CN102058938B CN 201010614813 CN201010614813A CN102058938B CN 102058938 B CN102058938 B CN 102058938B CN 201010614813 CN201010614813 CN 201010614813 CN 201010614813 A CN201010614813 A CN 201010614813A CN 102058938 B CN102058938 B CN 102058938B
Authority
CN
China
Prior art keywords
instrument
radiocurable
array
pixel
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN 201010614813
Other languages
Chinese (zh)
Other versions
CN102058938A (en
Inventor
A·龙
K·布朗
J·艾伦
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Elekta AB
Original Assignee
Elekta AB
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Elekta AB filed Critical Elekta AB
Priority to CN 201010614813 priority Critical patent/CN102058938B/en
Publication of CN102058938A publication Critical patent/CN102058938A/en
Application granted granted Critical
Publication of CN102058938B publication Critical patent/CN102058938B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Radiation-Therapy Devices (AREA)

Abstract

A panel image obtained during a concurrent radiotherapy period is often interfered by false images relative to pulses of MV energy. For a therapeutic radioactive pulse source, a pixel element array and a detector comprising a control circuit, each pixel element has a signal output end and an enabling input end and can be configured to send a signal under the triggering of the enabling input end through the signal output end and configured as an interpreter for receiving the signal output of the pixel elements, the interpreter is provided with a reset-controlling radiotherapy instrument; the imaging system has the advantages that the control circuit is suitable for resetting the interpreter after therapeutic radioactive pulses and the operation is prior to the enabling of at least one pixel of the array. Alternatively, the control circuit can prompt the pulse source to provide a plurality of pulses and then enables a plurality of pixels of the array. Actually, therapeutic pulses are grouped into short pulse clusters. Therefore, preferably, the plurality of pixels include almost all the pixels in the array.

Description

The imaging system that is used for ionizing radiation
The application be applicant Elekta AB on March 13rd, 2009 submit to, denomination of invention divides an application for the Chinese patent application No.200680055824.2's of " imaging system that is used for ionizing radiation ".
Technical field
The present invention relates to the imaging system for detection of ionizing radiation.
Background technology
Flat planar image is used in during radiotherapy and other use usually, to realize obtaining image from (for example) passes patient's ionizing radiation.Diagnosis imaging adopts kilovoltage (kV) radiation to obtain usually, and can be used as bidimensional image, or is used as a plurality of above-mentioned bidimensional images, in order to form the three dimensional representation by CR scanning.Radiotherapy trends towards in megavolt (MV) scope, and also can be used for obtaining launched field image (portal image).This is to pass this radiocurable image after the patient; Usually this image has the low quality that low contrast causes.However, anatomic characteristic is apparent in image, and these characteristics can be used to prove that (for example) patient is correctly disposed.
The radiogenic image of MV has intrinsic low contrast, and therefore, current do not have artefact to make in image to organize fuzzy be important.The MV source typically operates under duty factor is approximately 1/1000 pulse mode, therefore has sufficient chance to obtain data between pulse from the minority row of flat planar image.
Fig. 1 has shown the typical structure of flat-panel imager 10.Upper strata 12 is by forming at the scintillator that applies under x-ray 14.So produce light 16 and strike on photodiode and transistorized array 18, in above-mentioned photodiode and the transistor layout layer under being located immediately at upper strata 12.Array 18 is divided into single pixel, and each pixel is associated with independent photodiode.Clash on the photodiode of light in array, produce the electronic signal by the suitable gate of transistor.The electronic signal 20 that so produces is extracted from flat plate array via reading electronic device 22, to be formed for constructing the digit data stream 24 of described image.
Summary of the invention
We find, this type of launched field image is subject to the impact of the artefact relevant with the pulse of MV energy.When the MV pulse arrives, not only will cause the flicker of scintillator, also will list and read in transistor array and clash on electronic device and their material of ionization formation.Therefore this will produce other electronic signal, ignore scintillator and photodiode fully.We propose two kinds of methods can overcome this problem.
first aspect, therefore, we provide radiotherapy equipment, the pulse source and the flat panel detector that comprise the radiation of being used for the treatment of property, detector comprises control circuit, the pixel element array, each has signal output part and " enabling " input, and be set under by the described triggering that enables input via the signal output part release signal, and interpreter, this interpreter is set to receive the signal output of pixel element, interpreter has the control that resets, this control circuit is applicable to the interpreter that resets after the pulse of therapeutic radiation, before this operates at least one pixel that enables this array.
Therefore, interpreter stay open during resetting at treatment injure (on) or after activate.This will cause system's ignorance as the electric charge of the collection of pulse, and remove the artefact that therefrom produces.
Usually, the pixel element of this type of detector is by output signal work, and the total charge dosage of process shows the radiation of the total incident that is read since last this pixel in this signal.Because the radiation in pixel is incident, thus it cause ionization and as a result electric charge be retained.When pixel is in enabled state, flow of charge is through outfan and need be calculated.Like this, interpreter generally includes integrator, and in this case, resetting to control is provided so that the integrator zero clearing.Integrator is used to the electric current that enters photodiode is carried out integration, thereby measures the electric charge that has flow through.
Second solution of this problem is reevaluating in treatment accelerator operation pattern a kind of supposition behind.As mentioned above, aforesaid operations is approximately 1/1000 with duty factor and operates in pulse mode.Typically, this is near the 3 μ s pulses of every 3ms or this.
What treatment needed will be minimized total time ideally.As time goes by, it is tired that the patient becomes, and may move or inherence unintentionally motion will occur, and this means that long treatment will reduce clinical effectiveness.Further, the treatment time of reduction can allow more patient to receive treatment, therefore improves the clinical efficiency of instrument.Like this, treatment is completed in the shortest time as much as possible from requiring to pay, and can reach a conclusion thus, must have real extraordinary employing to be low to moderate the reason of 0.1% duty factor.Also will allow the improvement of ten times in clinical efficiency and the improvement that (is difficult to estimate) even be low to moderate 1% duty factor in clinical effectiveness.
This reason is to avoid the salvo of instrument thermal overload.The pulse that transmits comprises very high energy, and it is also huge making their needed energy.This energy must be dispersed, and (inevitably) some energy will the form with heat occur in instrument.Duty factor need to reduce in case the temperature of locking apparatus rises to unacceptable height.Selected duty factor is in this duty factor, to make the rate of heat addition that is input in device and the cooldown rate that provides be complementary.
We have realized that the existence of the time constant in the hot situation of device, in fact mean, in this equilibrium relation, the average duty factor in this time constant is important.If interim the growth then of duty factor reduces, instrument will begin heating, but cooling before surpassing acceptable temperature margin immediately.
Another aspect of the present invention, therefore, therefore we propose a kind of radiotherapy equipment, this instrument comprises the pulse source of therapeutic radiation, detector, and the control circuit that is used for this pulse source and this detector, this detector comprises the pixel element array, each has signal output part and " enabling " input, and be set under by the triggering that enables input via the signal output part release signal, control circuit is applicable to impel pulse source that a plurality of pulses are provided, and then enables a plurality of pixels of this array.
In fact, treatment injure is grouped into " train of pulse "---short impulse cluster (flurry of pulses).Within this time, the rate of heat addition of instrument will surmount its cooldown rate, and can raise by estimating temperature.Yet, will be and then cooling (downtime) period longer downtime of instrument.In this downtime, image can be collected from imaging panel.
Below that yes is preferred, namely these a plurality of pixels consist essentially of pixels all in this array.Yet before transmitting other trains of pulse, the part of collector panels is possible.
Usually, for the facility of analyzing, pel array is two-dimentional.In order to accelerate the speed of collection of images, the input that enables of one group of pixel is joined together, and therefore can enable simultaneously whole group.If by the row grouping, can be read simultaneously by so whole row in the 2D array for pixel.The output of every row pixel can be delivered to interpreter or other outfans via public outgoing route.
At present, canonical system has 400 maximum pulse rate to 600 pulses of per second.Using method of the present invention as above can allow this pulsation rate to rise to 1000 of per seconds or even 1500 pulses in the period that produces pulse.
This instrument can comprise the independent source of diagnostic radiation, or can by suitable treatment source generation, perhaps by the launched field image, perhaps produce more low-energy radiation by controlling this source for the radiation of imaging purpose.
Description of drawings
Embodiments of the invention will be described by example, with reference to the following drawings, wherein:
The schematic structure of Fig. 1 display panel imager;
Fig. 2 is presented at the detail view of the pixel of the group in this flat-panel imager;
The typical timing of the flat-panel imager of Fig. 3 displayed map 2;
Fig. 4 shows that being used for first of above-mentioned flat-panel imager revises timing;
Fig. 5 is presented at the typical timing of the flat-panel imager in the context that the MV pulse arrives;
Fig. 6 shows the timing of further correction; With
Timing in Fig. 7 displayed map 6 is for the impact of the hot property of accelerator.
The specific embodiment
Fig. 1 and 2 shows the imaging panel of standard basically.Fig. 1 is described, and demonstrates the vertical cross-section that passes single pixel.16 pixels of Fig. 2 display floater, although be the sub-fraction of entire panel, for explaining that the mode that a plurality of pixels are read is very sufficient.
As Fig. 2, therefore, pel array 26 is arranged in the mode of straight line, and pixel is lined up straight row and column.Therefore the cross point of specific row 28 and specific row 30 defines specific pixel 32.Each pixel has the transistor 34 that is associated with its outfan of gating, and each row has public " enabling " line 36, and this line activates the transistor 34 of each pixel in this row.
Every row have common output line 38, and the electric charge that this line allows to gather on each pixel is escaped to integrator 40, locate the outfan multiplexed (multiplexed) of it and other row at this.This just allows whole row to be read simultaneously.
Therefore scan control electronic device 42 sequentially enables every delegation, and whole row is read substantially at one time.Then integrator is reset, and next line is enabled.Timing is presented in Fig. 3.The signal RE that " exercises energy " is sent into each row successively.Be enabled and after the RE signal completed, " integrator resets " signal IR was sent out, thereby is that " n+1 " row is prepared this integrator at " n " row, the like.
Yet, between this does not consider or the MV pulse that arrives.As mentioned above, this pulse causes the ionization in the enable line 36 of being expert at, output lead 38, transistor 34 and integrator 40.All these will increase the electric charge of being collected by integrator, and will usually be enough to make the signal increase maybe may make signal saturated, and this will cause the distinguished white line that passes whole row.
Fig. 4 shows the timing arrangement of correction according to a particular embodiment of the invention.The figure illustrates megavolt pulse (MVP), this pulse occured in the indicated time for the treatment of control system (treatment control systems).The triggering signal of this pulse also offers the scan control electronic device, and the IR signal before this electronic device impels keeps " height " and be used for the RE signal being suspended, until after MVP stops.In fact, the IR signal extends as shown in 44, until MVP finishes, the RE signal is hung up during this period.Follow the IR signal ended, the RE signal continues their circulation.
According to this mode, the abnormal signal that is sent to integrator by MVP is allowed to disperse basically, and integrator is zero clearing after MVP, to prepare to receive the signal from next line.In fact most of panels will comprise some parasitic capacitances and resistance, and described resistance stops all electric charges to be removed from panel, but this technology will fully reduce this effect.
Fig. 5 and 6 shows the second embodiment of the present invention.Fig. 5 shows MVP and the RE track that is used for known system, but than the much longer time base that has in Fig. 3.Like this, some MVP trigger can be in sight, and the some RE that are accompanied by between them trigger.Usually, during each MVP triggered, system can read the several rows of panel.
Fig. 6 shows according to this invention, and how timing is modified.Described MVP triggers and is grouped into short bunch 46, does not have RE to trigger between them.After this bunch, RE triggers and restarts and be extended to (in this case) whole array to be read.After that, new MVP triggers and bunch is transmitted, and panel triggers sequence by new RE and rescaned.
This means, during this bunch 46 that MVP triggers, the rate of heat addition that is input in device is temporarily higher.Fig. 7 shows the steady statue for the heat input 48 of known system, and this state is the time averaging heat energy input by the MVP triggering for generating of Fig. 5.This produces stable temperature 50, and this temperature is such temperature, and in this temperature, the speed of heat input is balanced by the cooling system that is provided.Close on this steady heat input 48 shown be heat 52 (within a period of times) of input, this heat input 52 is produced by the correction timing in Fig. 6, well-regulated peak value 54 during MVP triggers bunches 46 wherein, the speed of heat input drops to 0. 56 between peak value.This has provided temperature curve Figure 58, have at the rising edge during peak value 54 along 60 and trailing edge between bunches 46 sawtooth along 58.
Far and away, if trigger higher rate maintenance in long-time that bunches 46 MVP triggers, this instrument is with thermal overload.Yet the critical temperature condition needs certain hour to arrive, and must just can be elevated to higher temperature by using sufficient thermal energy as the thermal mass of installing.Therefore, exist to be used for time of bunches 46; This moves MVP and triggers to produce the gap, and panel is read in this gap.This means, or the artefact that does not have MVP to bring out in image, or artefact is limited to the first row that is read.In the later case, this row can be arranged on edge, thereby is left in the basket.
Far and away, two embodiment can be combined, even if the first embodiment is used to prevent that any artefact from appearing at the first row of the image that reads according to the second embodiment.However, they still allow independent utility.
This will yes holds intelligiblely, and only otherwise depart from aim of the present invention, many variations can be implemented in the above-described embodiments.

Claims (11)

1. radiocurable instrument comprises pulse source, the detector of therapeutic radiation and is used for the control circuit of described pulse source and described detector,
Described detector comprises the pixel element array, and each pixel element has signal output part and " enabling " input, and is set under by the described triggering that enables input via described signal output part release signal,
Described control circuit is applicable to impel described pulse source that a plurality of pulses are provided, and then enables a plurality of pixels of this array.
2. radiocurable instrument as claimed in claim 1, wherein, described a plurality of pixels comprise pixels all in array.
3. radiocurable instrument as described in any one in aforementioned claim 1 to 2, wherein, described array is two-dimentional.
4. radiocurable instrument as claimed in claim 3, wherein, the input that enables of pixel groups is joined together, and therefore enables simultaneously whole group.
5. radiocurable instrument as claimed in claim 4, wherein, in the 2D array, described pixel is by the row grouping.
6. radiocurable instrument as claimed in claim 4, wherein, the output of the signal of a plurality of pixels is delivered to integrator via public outgoing route, and each pixel belongs to different groups.
7. radiocurable instrument as described in any one in claim 1 to 2, wherein, described pixel element output signal, in this signal, the total electrical charge of process shows the total incident radiation that begins from predetermined situations.
8. radiocurable instrument as described in any one in claim 1 to 2, wherein, the pulse recurrence frequency in source changes.
9. radiocurable instrument as described in any one in claim 1 to 2, wherein, the pulse recurrence frequency in source is 1000 pulses of per second at least.
10. radiocurable instrument as described in any one in claim 1 to 2, wherein, the pulse recurrence frequency in source is at least 1500 pulses of per second.
11. radiocurable instrument as described in any one in claim 1 to 2 further comprises the independent source of diagnostic radiation.
CN 201010614813 2006-09-13 2006-09-13 Imaging system for ionizing radiation Active CN102058938B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 201010614813 CN102058938B (en) 2006-09-13 2006-09-13 Imaging system for ionizing radiation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 201010614813 CN102058938B (en) 2006-09-13 2006-09-13 Imaging system for ionizing radiation

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
CN2006800558242A Division CN101516445B (en) 2006-09-13 2006-09-13 Radiation therapeutic instrument

Publications (2)

Publication Number Publication Date
CN102058938A CN102058938A (en) 2011-05-18
CN102058938B true CN102058938B (en) 2013-06-19

Family

ID=43994555

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 201010614813 Active CN102058938B (en) 2006-09-13 2006-09-13 Imaging system for ionizing radiation

Country Status (1)

Country Link
CN (1) CN102058938B (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US680858A (en) * 1899-09-11 1901-08-20 Milton A Hamilton Acetylene-gas generator.
CN1763513A (en) * 2004-10-01 2006-04-26 佳能株式会社 Radiographic imaging apparatus and method
CN1825205A (en) * 2005-02-24 2006-08-30 佳能株式会社 Radiography apparatus, radiography system, and control method thereof

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US680858A (en) * 1899-09-11 1901-08-20 Milton A Hamilton Acetylene-gas generator.
CN1763513A (en) * 2004-10-01 2006-04-26 佳能株式会社 Radiographic imaging apparatus and method
CN1825205A (en) * 2005-02-24 2006-08-30 佳能株式会社 Radiography apparatus, radiography system, and control method thereof

Also Published As

Publication number Publication date
CN102058938A (en) 2011-05-18

Similar Documents

Publication Publication Date Title
CN103126695B (en) Radiographic image detector and control method thereof
CN104582574B (en) Electronic type radiography systems and signal relay device
US4383327A (en) Radiographic systems employing multi-linear arrays of electronic radiation detectors
CN104641257B (en) Radiological image detection
CN103239245B (en) Radiation imaging and control method thereof, and radiation imaging system
US4878234A (en) Dental x-ray diagnostics installation for producing panorama slice exposures of the jaw of a patient
EP0724729B1 (en) Thin-film, flat panel, pixelated detector array for real-time digital imaging and dosimetry of ionizing radiation
CN104068882B (en) Radiological image detection apparatus and its operating method and radiation imaging system
EP1167999A1 (en) Multi-element-amorphous-silicon-detector-array for real-time imaging and dosimetry of megavoltage photons and diagnostic x-rays
CN106550527A (en) For the auto-exposure control of x-ray imaging
CN100507604C (en) Radimeter for adjusting offset component
JP2016140762A (en) Panoramic imaging using multi-spectral x-ray source
KR102338713B1 (en) Automatic exposure control method and automatic exposure control component system
CN102058938B (en) Imaging system for ionizing radiation
CN101516445B (en) Radiation therapeutic instrument
CN102271585A (en) Method for x-ray imaging using scattered radiation
USRE32164E (en) Radiographic systems employing multi-linear arrays of electronic radiation detectors
KR20150027636A (en) Method for elimination of residual charge, X-ray imaging method and apparatus using the method
CN104023637B (en) Radiographic image camera chain and radiation line detector
US9635748B2 (en) Systems and methods for high-speed radiography with high resolution imaging of large-area fields
USRE32779E (en) Radiographic systems employing multi-linear arrays of electronic radiation detectors
CN106580358A (en) Tomography system and tomoscan control circuit thereof
EP3469789B1 (en) High frame capture rate synchronization with streaming mode
US20210330277A1 (en) Software synchronization for bedside dynamic imaging
Yoo et al. Fast visible camera diagnostic for dual shattered pellet injections at KSTAR

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant