RU2015122382A - Сцинтилляционный материал - Google Patents
Сцинтилляционный материал Download PDFInfo
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- RU2015122382A RU2015122382A RU2015122382A RU2015122382A RU2015122382A RU 2015122382 A RU2015122382 A RU 2015122382A RU 2015122382 A RU2015122382 A RU 2015122382A RU 2015122382 A RU2015122382 A RU 2015122382A RU 2015122382 A RU2015122382 A RU 2015122382A
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- 239000000463 material Substances 0.000 title claims 13
- 230000003287 optical effect Effects 0.000 claims 16
- 238000012879 PET imaging Methods 0.000 claims 6
- 230000005251 gamma ray Effects 0.000 claims 5
- 238000000034 method Methods 0.000 claims 3
- 238000002600 positron emission tomography Methods 0.000 claims 3
- 230000002285 radioactive effect Effects 0.000 claims 3
- 239000004065 semiconductor Substances 0.000 claims 3
- 229910052684 Cerium Inorganic materials 0.000 claims 2
- GWXLDORMOJMVQZ-UHFFFAOYSA-N cerium Chemical compound [Ce] GWXLDORMOJMVQZ-UHFFFAOYSA-N 0.000 claims 2
- 239000002223 garnet Substances 0.000 claims 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical group [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims 1
- 238000010521 absorption reaction Methods 0.000 claims 1
- 239000000919 ceramic Substances 0.000 claims 1
- 238000003384 imaging method Methods 0.000 claims 1
- 238000005259 measurement Methods 0.000 claims 1
- 239000002245 particle Substances 0.000 claims 1
- 230000035945 sensitivity Effects 0.000 claims 1
- 229910052710 silicon Inorganic materials 0.000 claims 1
- 239000010703 silicon Substances 0.000 claims 1
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- G01T1/16—Measuring radiation intensity
- G01T1/20—Measuring radiation intensity with scintillation detectors
- G01T1/2006—Measuring radiation intensity with scintillation detectors using a combination of a scintillator and photodetector which measures the means radiation intensity
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Claims (24)
1. Сцинтилляционный материал гранат с по существу керамической или поликристаллической структурой и временем затухания менее чем 300 нс, имеющий состав, представленный формулой: Gd3-x-yLuxCey)(Al5-zGaz-aLua)O12; причем x находится в диапазоне от 0 до 0,6, причем y находится в диапазоне от 0,003 до 0,03 и соответствует количеству церия в диапазоне от 0,1 мол % до 1,0 мол %, причем z находится в диапазоне от 1,5 до 3,5, причем a находится в диапазоне от 0 до 0,3.
2. Сцинтилляционный материал по п. 1, причем сцинтилляционным материалом-основой является гранат, имеющий состав, представленный формулой: (Gd-2,7-yLu0,3Cey)Al2,5Ga2,47Lu0,03)O12, причем y находится в диапазоне от 0,003 до 0,03 и соответствует количеству церия в диапазоне от 0,1 мол % до 1,0 мол %.
3. Сцинтилляционный материал по п. 2, имеющий время затухания менее чем 300 нс.
4. Сцинтилляционный материал по п. 1, причем состав регулируется так, что плотность состава находится в диапазоне от 5 до 8 г/см3.
5. Детектор гамма-фотонов, содержащий сцинтилляционный материал по п. 1 в оптической связи с оптическим детектором.
6. Детектор гамма-фотонов по п. 5, причем оптический детектор (3) имеет активную площадь менее чем 5 см2.
7. Детектор гамма-фотонов по п. 5, причем площадь приема гамма-фотонов составляет менее чем 5 см2.
8. Детектор гамма-фотонов по п. 5, причем оптический детектор является детектором с фотоэлектронным умножителем (ФЭУ).
9. Детектор гамма-фотонов по п. 8, причем пик оптической чувствительности детектора с ФЭУ находится в диапазоне от 450 нм до 700 нм.
10. Детектор гамма-фотонов по п. 5, причем оптический детектор является твердотельным полупроводниковым оптическим детектором.
11. Детектор гамма-фотонов по п. 10, причем твердотельный полупроводниковый оптический детектор является кремниевый оптическим детектором, имеющим структуру n+ - i - p+, и n+ слой расположен ближе к границе раздела со сцинтилляционным материалом, чем p+ слой.
12. Система визуализации ПЭТ (позитронно-эмиссионной томографии), имеющая поле сканирования и содержащая по меньшей мере два детектора гамма-фотонов по п. 5, причем детекторы гамма-фотонов расположены радиально вокруг поля сканирования и выполнены с возможностью принимать гамма-фотоны из упомянутого поля сканирования.
13. Система визуализации ПЭТ с измерением времени пролета частиц (TOF) по п. 12.
14. Система визуализации ПЭТ, имеющая поле сканирования и содержащая:
множество детекторов гамма-фотонов, расположенных радиально вокруг поля сканирования и выполненных с возможностью принимать гамма-фотоны из упомянутого поля сканирования;
причем каждый детектор гамма-фотонов содержит сцинтилляционный материал по п. 1 в оптической связи с оптическим детектором с фотоэлектронным умножителем;
причем система визуализации ПЭТ имеет площадь считывания гамма-фотонов менее чем 33 см2.
15. Система визуализации ПЭТ, имеющая поле сканирования и содержащая:
множество детекторов гамма-фотонов, расположенных радиально вокруг поля сканирования и выполненных с возможностью принимать гамма-фотоны из упомянутого поля сканирования;
причем каждый детектор гамма-фотонов содержит сцинтилляционный материал по п. 1 в оптической связи с твердотельным полупроводниковым оптическим детектором;
причем система визуализации ПЭТ имеет площадь считывания гамма-фотонов менее чем 10 см2.
16. Способ создания изображения ПЭТ, указывающего на распределение радиоактивной метки в пределах поля сканирования, причем способ содержит: введение радиоактивной метки субъекту,
ожидание в течение заранее заданного периода поглощения после введения радиоактивной метки и отображение по меньшей мере части тела упомянутого субъекта с помощью системы визуализации ПЭТ по п. 12.
17. Способ обнаружения по меньшей мере одного гамма-фотона, содержащий этапы: приема по меньшей мере одного гамма-фотона с помощью сцинтилляционного материала по п. 1; обнаружение сцинтилляционного света, сгенерированного упомянутым сцинтилляционным материалом, с помощью упомянутого оптического детектора в оптической связи с упомянутым сцинтилляционным материалом и генерирование электрического выходного сигнала от упомянутого оптического детектора в ответ на по меньшей мере один принятый гамма-фотон.
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EP3197983B1 (en) * | 2014-09-25 | 2023-06-07 | Koninklijke Philips N.V. | Detection device for detecting gamma or x-ray radiation |
US9606245B1 (en) | 2015-03-24 | 2017-03-28 | The Research Foundation For The State University Of New York | Autonomous gamma, X-ray, and particle detector |
JP6762949B2 (ja) * | 2015-09-18 | 2020-09-30 | 株式会社東芝 | 中性子検出用シンチレータアレイおよび中性子の検出方法 |
US20170090042A1 (en) * | 2015-09-30 | 2017-03-30 | Varian Medical Systems, Inc. | Method for fabricating pixelated scintillators |
US10000698B2 (en) * | 2016-03-08 | 2018-06-19 | Lawrence Livermore National Security, Llc | Transparent ceramic garnet scintillator detector for positron emission tomography |
WO2017192554A1 (en) * | 2016-05-02 | 2017-11-09 | Daniel Gagnon | Method and apparatus for performing co-planar and simultaneous spectral ct and pet imaging |
US10054697B1 (en) * | 2017-04-11 | 2018-08-21 | Consolidated Nuclear Security, LLC | Device and method for locating a radiation emitting source via angular dependence using a single detection crystal |
JP2019102456A (ja) | 2017-11-30 | 2019-06-24 | ガタン インコーポレイテッドGatan Inc. | 電子顕微鏡法のための高密度高速発光体 |
CN109342482B (zh) * | 2018-11-16 | 2024-05-28 | 深圳市福瑞康科技有限公司 | 一种闪烁检测装置、方法及其应用 |
CN109884684B (zh) * | 2019-01-10 | 2020-09-15 | 中国科学院高能物理研究所 | 一种用于pet闪烁晶体性能测试的电子学数据处理方法及*** |
WO2020150344A1 (en) * | 2019-01-16 | 2020-07-23 | Schott Corporation | Chalcogenide glass and glass ceramic scintillators |
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US6458295B1 (en) * | 1997-12-24 | 2002-10-01 | Hitachi Medical Corporation | Phosphors, and radiation detectors and X-ray CT unit made by using the same |
US6552348B2 (en) * | 1999-12-14 | 2003-04-22 | Regents Of The University Of California | Apparatus and method for breast cancer imaging |
JP4683719B2 (ja) * | 2000-12-21 | 2011-05-18 | 株式会社日立メディコ | 酸化物蛍光体及びそれを用いた放射線検出器、並びにx線ct装置 |
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