Direct conversion radiation detector

Patent metadata

Field	Value
Publication number	US-2018106910-A1
Application number	US-201615501193-A
Country	US
Kind code	A1
Filing date	Jun 28, 2016
Priority date	Jul 9, 2015
Publication date	Apr 19, 2018
Grant date	—

Abstract

The present invention relates to a direct conversion radiation detector for wherein the direct conversion material comprises a garnet with a composition of Z 3 (Al x Ga y )O 12 :Ce, wherein Z is Lu, Gd, Y, Tb or combinations thereof and wherein y is equal to or greater than x; and preferably Z comprises Gd. Suitable garnets directly convert radiation, such as x-rays or gamma-rays, into electronic signals. Preferably photoluminescence of the garnet is low or absent. The detector is particularly suitable for use in x-ray imaging devices, such as computed tomography. In some embodiments photoluminescence of garnets might be used to construct a hybrid direct-indirect conversion detector, which may be particularly suitable for use with Time-of-Flight PET.

First claim

1 . A direct conversion radiation detector comprising:
a direct conversion layer comprising a direct conversion material for directly converting incoming radiation from a radiation source into electron and hole pairs; a first electrode mounted on the direct conversion layer facing the radiation source; a second electrode mounted on an opposite side of the direct conversion layer compared to the first electrode; and means for applying an electrical potential between the first electrode and the second electrode, characterized in that the direct conversion material comprises a garnet with a composition of Z 3 (Al x Ga y ) 5 O 12 :Ce, wherein Z is Lu, Gd, Y, Tb or combinations thereof and wherein y is equal to or greater than x; and preferably Z comprises Gd.

2 . The direct conversion radiation detector according to claim 1 , wherein the second electrode is pixelated.

3 . The direct conversion radiation detector according to claim 1 , further comprising a photosensor mounted behind the second electrode with respect to the direct conversion layer for converting visible light formed in the direct conversion layer to an electronic signal, wherein the second electrode is transparent to visible light and wherein y is preferably between 0.4 and 0.6, more preferably y is about 0.5, and/or wherein the garnet is preferably a garnet wherein Z comprises Gd and Lu with a Gd:Lu ratio of about 2:1.

4 . The direct conversion radiation detector according to claim 1 , further comprising an integrated circuit for processing electronic signals generated in the direct conversion radiation detector.

5 . The direct conversion radiation detector according to claim 4 , further comprising a transparent re-routing layer for re-routing each pixel of the pixelated electrode to the integrating circuit.

6 . A radiation imaging method, comprising the steps of:
emitting a radiation beam from a radiation source; detecting the emitted radiation beam with a direct conversion radiation detector according to claim 1 ; generating a first electronic signal indicative of a number of detected charge carriers generated in the direct conversion layer.

7 . The radiation imaging method according to claim 6 , wherein the direct conversion radiation detector is a direct conversion radiation detector and a first electronic signal is generated for each detector pixel of the pixelated second electrode.

8 . The radiation imaging method according to claim 6 , wherein the direct conversion radiation detector is a direct conversion radiation detector (, further comprising the step of:
generating a second electronic signal indicative of a number of detected electrons generated in the photosensor.

9 . The radiation imaging method according to claim 7 , wherein the radiation source is a decaying radioactive material, further comprising the following steps:
detecting two simultaneously formed photons with at least the radiation detector; determining a difference in detection time between the two simultaneously formed photons; generating a timestamp based on the determined difference in detection time, wherein the step of generating a first electronic signal includes using the generated timestamp as input.

10 . The radiation imaging method according to claim 6 , further comprising the step of:
generating image data based on the first electronic signal.

11 . The radiation imaging method according to claim 8 , further comprising the steps of:
generating image data based on the first electronic signal and on the second electronic signal.

12 . The radiation imaging method according to claim 10 , further comprising the step of:
displaying the image data.

13 . An imaging system comprising a direct conversion radiation detector according to claim 1 .

14 . The imaging system according to claim 13 , selected from a group comprising X-ray imaging device, computed tomography imaging device, preferably a spectral computed tomography imaging device, position emission tomography imaging device, preferably a time-of-flight positron emission tomography imaging device, single-photon emission computed tomography device, or combinations thereof.

Assignees

• Koninklijke Philips Nv

Inventors

• Verbakel Frank
• Ronda Cornelis Reinder
• Wieczorek Herfried Karl

Classifications

• G01T1/241 Primary

  Electrode arrangements, e.g. continuous or parallel strips or the like · CPC title

• G01T1/24 Primary

  with semiconductor detectors · CPC title

• G01T1/2985

  In depth localisation, e.g. using positron emitters; Tomographic imaging (longitudinal and transverse section imaging; apparatus for radiation diagnosis sequentially in different planes, steroscopic radiation diagnosis); (using external radiation sources A61B6/02) · CPC title

• G01T1/202 Primary

  the detector being a crystal · CPC title