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CN106291656A - Prompt fission gammas's imaging system - Google Patents

Prompt fission gammas's imaging system
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Publication number
CN106291656A
CN106291656ACN201610614625.6ACN201610614625ACN106291656ACN 106291656 ACN106291656 ACN 106291656ACN 201610614625 ACN201610614625 ACN 201610614625ACN 106291656 ACN106291656 ACN 106291656A
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gamma
particle
gammaphoton
detector
probe
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CN201610614625.6A
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汪金龙
雷海
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Abstract

The invention discloses prompt fission gammas's imaging system, by measuring prompt fission gammas's photon, measure particle range and beam position in patient body in real time, make the line inciding in patient body visible.The present invention includes following sections: longitudinal gamma detector (1), laterally gamma detector (2), detector is formed detector array by multiple gamma-ray probes (3), and each gamma-ray probe is made up of scintillation crystal (4), photoelectric sensor (5) and grating (6).Cylindrical PMMA material (7) simulated human tissue, tumor (8) is on its interior, particle beam (9) passes human body simulation tissue bombardment to tumor, inspire gammaphoton on its path passed, by measuring the distribution of gammaphoton, gamma detector determines that the range of particle and beam position are distributed.This system can be widely used for proton heavy particle therapy terminal.

Description

Prompt fission gammas's imaging system
Technical field
Belong to beam diagnostics and fields of measurement, be applied particularly to proton heavy ion medical terminal, measure line in real time in diseaseRange in human body, generates beam pattern picture.Can also be used on other types accelerator installation, and section's grinding device.
Background technology
Proton heavy particle therapy is a kind of precisely pencil beam scanning that cancer treatment method, especially last decade grow upMethod, intensity modulated therapy method, the premise that these methods are achieved is particle being accurately positioned in patient body.A kind of basic sideCase is to optimize Beam Transport Systems, treatment plan, is accurately positioned treatment chair or therapeutic bed, comes by optimizing equipment and software precisionRealize precisely treatment.But a lot of uncertain factors still can affect the range of particle and the breathing of the distribution of dosage, such as patient,The inhomogeneities of tissue, focus self mobile etc..
Summary of the invention
It is an object of the invention to design a kind of prompt fission gammas's imaging system, by measuring prompt fission gammas's photon, measure in real timeParticle range and beam position in patient body, make the line inciding in patient body visible.This system can be widely used for protonHeavy particle therapy terminal.
As it is shown in figure 1, prompt fission gammas's imaging system includes following sections: longitudinal gamma detector (1), horizontal gamma is visitedSurveying device (2), detector is formed detector array by multiple gamma-ray probes (3), and each gamma-ray probe is by scintillation crystal (4), photoelectricitySensor (5) and grating (6) composition.Cylindrical PMMA material (7) simulated human tissue, tumor (8) is on its interior, particle beamStream (9), through human body simulation tissue bombardment in tumor, inspires gammaphoton on its path passed, and gamma detector leads toCross the distribution measuring gammaphoton to determine range and the beam position distribution of particle.
Longitudinal gamma detector (1) is positioned at cylindrical PMMA material (7) top, and spacing is 60mm;Laterally gamma detector(2) being positioned at cylindrical PMMA material (7) rear portion, spacing is 110mm.
It is logical with substance in vivo interaction radiation gammaphoton, such as proton that particle (proton and heavy ion) injects tissueCross reaction16O(p, p*)16O* launches 6.129 MeV, 6.916 MeV, the gammaphoton of 7.115 MeV energy.Gammaphoton producesVolume is followed at the bragg peak trailing edge of proton end-of-range and is drastically declined, and determines proton range by measuring gammaphoton,As in figure 2 it is shown, the cylindrical PMMA material of a diameter of 200mm of the Proton-Induced Reactions of 160MeV, long 400mm.Gammaphoton yieldIt is scattered in corresponding relation with particle, the distribution of gammaphoton can be measured to measure the distribution of line.
The critical piece of gamma-ray probe (3) is scintillation crystal (4) and photoelectric sensor (5), and scintillation crystal is by incident galHorse photon excitation, produces photoelectron, photoelectric sensor output signals, and backend electronics learns position and the energy letter of record gammaphotonBreath.
Scintillation crystal selection principle is that photoyield is high, and decay constant is little, and refractive index is low, is difficult to deliquescence, easily cuts into littleBlock.Fig. 3 lists several optional crystal parameter, reasonable such as LYSO crystal, LaBr3: Ce crystal.
Photoelectric sensor selection principle is that the rise time is short, biases low, and volume is little, is easily integrated as multichannel array.Fig. 4List several optional sensor parameters, reasonable selection such as avalanche photodide (APD), silicon photomultiplier(SiPM)。
As it is shown in figure 5, the gammaphoton (61) incident in order to only receive vertical direction, around scintillator, there is provision of lightGrid (6).Grating is in close contact with scintillator.In order to stop lateral incident high energy gammaphoton (63), grating not only to wrap entirelyWrap up in crystal, also long than crystal.Crystal section 9mm × 9mm in the present embodiment, long 20mm, grating wall thickness 1mm, long 70mm.
Owing to offspring (62) and grating material effect also can produce gammaphoton (621 ~ 622), this part gamma lightSon has part (621) to be directly incident in probe, but the energy of this part gammaphoton is relatively low, generally less than 5 MeV, such as figureShown in 6.Therefore the window energy of gamma detector elects 5 MeV as.I.e. only has the energy gammaphoton just meeting more than window energyBy detector record.
Longitudinal gamma detector (1) measures the range of particle, as it is shown in fig. 7, longitudinal gamma detector (1) is by multipleThe array that gamma-ray probe (3) forms, each probe mark is P (X, Y, Z), and X, Y, Z correspond in this probe crystal geometryThe heart space coordinates, matrix initial point is positioned at the particle incidence point in tissue.Each probe sectional dimension pixel is the least, surveysThe precision of amount is the highest.The present embodiment longitudinal direction gamma detector is 9 × 40 probes.
Owing to the transmitting of gammaphoton is isotropic, the path that therefore particle can be passed is considered as line source,In the case of being not added with grating, each probe will receive the gammaphoton from each point, and probe 1 and 2 all receives A and B point and sends outThe gammaphoton gone out, the genesis analysis of gamma detector gained will be unable to determine the range of particle, as shown in Figure 8.
In order to only measure the gammaphoton of vertical incidence, need to be arranged around grating at probe, the higher atomic number of gratingThe metal of number is made, and can effectively stop gammaphoton, uses tantalum in the present embodiment.The gamma distribution such as figure measured after grating is setShown in 9, pop one's head in 1 and receive the gammaphoton that A point sends, pop one's head in 2 and receive the gammaphoton that B point sends, therefore, it is possible to measureThe range of particle.
One group of parallel gamma light of any incident direction can be selected in principle.To select to be perpendicular to the parallel of beam directionLight is optimal, can reduce processing cost and installation difficulty;If selecting the directional light being more than 90 ° with line angle, then can reduce heatNeutronic noise, in the case of this, probe installation direction is parallel to gammaphoton.
Laterally gamma detector (2) measures the cross direction profiles of end-of-range particle, is made up of 9 × 9 probes, thus measuresThe cross section of particle range end line.As shown in Figure 10.
Longitudinal gamma detector (1) can be used for measuring the lateral cross section of line, as shown in figure 11, given longitudinal coordinateValue Zi, takes probe P (-4,15, Zi) and can provide grain at longitudinal degree of depth Zi to the data that P (4,15, Zi) nine pops one's head inHorizontal (X) distribution cross section of son.To the cross section of Y-direction at detection Zi, also needing to increase by one group of detector, its position is perpendicular to indulgeTo gamma detector (1).
Comprehensive longitudinal gamma detector (1), the data of horizontal gamma detector (2) can obtain line reality in human bodyTime image information, including the range of particle, beam cross section.As shown in Figure 12 and Figure 13.By image combining method, show in real timeLine 3-D view in patient body, as shown in figure 14.
It will be apparent to those skilled in the art that can technical scheme as described above and design, make other variousCorresponding change and deformation, and all these changes and deformation all should belong to the claims in the present invention protection domain itIn.
Accompanying drawing explanation
Fig. 1-prompt fission gammas's imaging system schematic diagram;
Fig. 2-bragg peak and gammaphoton profiles versus;
Fig. 3-scintillation crystal parameter list;
Fig. 4-photoelectric sensor parameter list;
Fig. 5-gamma-ray probe;
Fig. 6-100MeV neutron is beaten tantalum and is produced photons spectrum;
Fig. 7-longitudinal direction gamma detector array;
Fig. 8-no-raster measures gammaphoton distribution;
Fig. 9-have grating measuring gammaphoton to be distributed;
Figure 10-horizontal gamma detector;
Figure 11-horizontal (X) distribution cross section;
Figure 12-beam pattern is as XZ cross section;
Figure 13-particle range end beam pattern is as XY cross section;
Figure 14-line 3-D view.

Claims (10)

CN201610614625.6A2016-08-012016-08-01Prompt fission gammas's imaging systemPendingCN106291656A (en)

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Cited By (11)

* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
CN108828647A (en)*2018-05-302018-11-16中国原子能科学研究院It is a kind of for measuring the device of low energy ion beam streamer dose rate and uniformity
CN109974811A (en)*2019-04-152019-07-05上海沃纳机电设备有限公司 An array radiation level gauge and its measurement method
CN109974810A (en)*2019-04-152019-07-05上海沃纳机电设备有限公司A kind of more fronts radiation level-sensing device and its measurement method
CN110215619A (en)*2018-03-032019-09-10彭浩Proton intelligent online monitors system and method
CN110772720A (en)*2018-07-302020-02-11汪金龙Adaptive particle radiotherapy system based on prompt radiation-cone beam computed tomography combined guidance
CN110787376A (en)*2019-11-292020-02-14合肥中科离子医学技术装备有限公司Tumor patient positioning system based on proton imaging
CN112326708A (en)*2020-10-202021-02-05汪金龙Human tissue density and element composition reconstruction algorithm based on prompt gamma spectrum
US11506801B2 (en)2018-10-102022-11-22Ebamed SaPrompt gamma monitor for hadron therapy
US12156760B2 (en)2019-11-142024-12-03Ebamed SaCardiac phase gating system for radiation therapy
US12311200B2 (en)2020-12-232025-05-27Ebamed SaMultiplanar motion management system
US12318632B2 (en)2017-11-162025-06-03Ebamed SaHeart arrhythmia non-invasive treatment device and method

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US20090242838A1 (en)*2008-03-282009-10-01Consiglio Nazionale Delle Ricerche (Cnr)Method for obtaining a scintillation structure
US20110186720A1 (en)*2008-07-032011-08-04Yves JongenDevice And Method For Particle Therapy Verification
US8049176B1 (en)*2008-12-122011-11-01Jefferson Science Assocates, LLCMethod and apparatus for real time imaging and monitoring of radiotherapy beams
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Cited By (14)

* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
US12318632B2 (en)2017-11-162025-06-03Ebamed SaHeart arrhythmia non-invasive treatment device and method
CN110215619A (en)*2018-03-032019-09-10彭浩Proton intelligent online monitors system and method
CN110215619B (en)*2018-03-032022-03-08彭浩Intelligent proton on-line monitoring system
CN108828647A (en)*2018-05-302018-11-16中国原子能科学研究院It is a kind of for measuring the device of low energy ion beam streamer dose rate and uniformity
CN110772720A (en)*2018-07-302020-02-11汪金龙Adaptive particle radiotherapy system based on prompt radiation-cone beam computed tomography combined guidance
US11506801B2 (en)2018-10-102022-11-22Ebamed SaPrompt gamma monitor for hadron therapy
CN109974811A (en)*2019-04-152019-07-05上海沃纳机电设备有限公司 An array radiation level gauge and its measurement method
CN109974810A (en)*2019-04-152019-07-05上海沃纳机电设备有限公司A kind of more fronts radiation level-sensing device and its measurement method
CN109974810B (en)*2019-04-152024-08-09上海沃纳机电设备有限公司Multi-array-surface radiation level gauge and measuring method thereof
US12156760B2 (en)2019-11-142024-12-03Ebamed SaCardiac phase gating system for radiation therapy
CN110787376A (en)*2019-11-292020-02-14合肥中科离子医学技术装备有限公司Tumor patient positioning system based on proton imaging
CN112326708A (en)*2020-10-202021-02-05汪金龙Human tissue density and element composition reconstruction algorithm based on prompt gamma spectrum
CN112326708B (en)*2020-10-202023-10-24汪金龙Human tissue density and element composition reconstruction algorithm based on instantaneous gamma spectrum
US12311200B2 (en)2020-12-232025-05-27Ebamed SaMultiplanar motion management system

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Application publication date:20170104


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