# US 9,753,156 B2 · Detector > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 9,753,156 B2 - Document ID: US9753156B2 - Status: Granted - Kind: B2 - Application number: 14/768,231 - Filed: 2014-02-28 - Published: 2015-12-17 - Granted: 2017-09-05 - Earliest claimed: 2013-03-01 - Assignees: Koninklijke Philips N.V. - Applicants: Koninklijke Philips N.V. - Inventors: Frank Verbakel; Klaus Juergen Engel; Antonius Johannes Maria Nellissen; Herfried Karl Wieczorek; Eric Cornelius Egbertus Van Grunsven; Ira Micah Blevis; Roger Steadman Booker - Web page: https://patentgrep.com/patent/US9753156B2 ## CPC - G01T 1/244: {Auxiliary details, e.g. casings, cooling, damping or insulation against damage by, e.g. heat, pressure or the like} - G01N 23/02: by transmitting the radiation through the material - G01T 1/24: with semiconductor detectors - G01T: MEASUREMENT OF NUCLEAR OR X-RADIATION (radiation analysis of materials, mass spectrometry G01N23/00; tubes for determining the presence, intensity, density or energy of radiation or particles H01J47/00) - G01N: INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES (measuring or testing apparatus or processes other than immunoassay, involving enzymes or microorganisms C12M, C12Q) ## Abstract The invention relates to a detector (6) for detecting radiation, especially x-ray radiation used in a computed tomography system. The detector comprises a direct conversion material (9) for converting radiation into electrons and holes, which are used for generating an electrical detection signal. The direct conversion material is illuminated with illumination light being broadband visible and/or broadband infrared light for reducing, in particular, eliminating, a polarization of the direct conversion material, which may occur when being traversed by the radiation to be detected and which may reduce the detection performance. By reducing the polarization of the direct conversion material the detection performance can be improved. ## Claims ### Claim 1 A detector for detecting radiation, the detector comprising: an anode, a cathode and an intermediate direct conversion material for converting radiation into electrons and holes, wherein the electrons are collectable by the anode, the intermediate direct conversion material is disposed between the anode and the cathode, the intermediate direct conversion material comprises an incidence surface, and the cathode is arranged on the incidenece surface; a detection signal generator for generating a detection signal depending on the collected electrons; an illuminator for illuminating the intermediate direct conversion material with illumination light being broadband visible and/or broadband infrared light, wherein the illuminator comprises: a diffractive plate with macro structures; a light source, located outside of the radiation, configured to emit illumination light from outside a path of the radiation; and coupling element that couples the illumination light through a side surface of the diffractive plate into the diffractive plate, where the illumination light is coupled out of the macro structures and traverses opening in the cathode to the intermediate direct conversion material; and wherein wavelengths of the illumination light include a band of wavelengths at least 100 nm broad. ### Claim 2 (depends on 1) The detector as defined in claim 1, wherein the diffractive plate diffracts the illumination light before traversing the cathode. ### Claim 3 (depends on 1) The detector as defined in claim 1, wherein the illuminator is a separate element such that it is movable with respect to the anode, the cathode and the direct conversion material. ### Claim 4 (depends on 1) The detector as defined in claim 1, wherein the illuminator is adapted to illuminate the direct conversion material in an intensity modulated mode. ### Claim 5 (depends on 1) The detector as defined in claim 1, wherein the illuminator is adapted to illuminate the direct conversion material depending on the generated detection signal. ### Claim 6 (depends on 1) The detector as defined in claim 1, wherein the detector further comprises a polarization degree determination unit for determining a polarization degree value being indicative of a degree of polarization of the direct conversion material, wherein the illuminator is adapted to illuminate the direct conversion material depending on the polarization degree value. ### Claim 7 (depends on 6) The detector as defined in claim 6, wherein the polarization degree determination unit is adapted to measure the time needed by electrons to move from the cathode to the anode and to determine the polarization degree value depending on the measured time. ### Claim 8 (depends on 1) A projection data generation system for generating projection data of an object, the system comprising: a radiation source for providing radiation for traversing the object, the detector as defined in claim 1 for detecting the radiation, after having traversed the object, for generating a detection signal depending on the detected radiation and for generating the projection data depending on the generated detection signal. ### Claim 9 (depends on 1) A detection method for detecting radiation by using a detector as defined in claim 1, the detection method comprising: converting radiation into electrons and holes by the intermediate direct conversion material arranged between the anode and the cathode, wherein the electrons are collected by the anode; generating the detection signal depending on the collected electrons by the detection signal generator; illuminating the direct conversion material with illumination light being broadband visible and/or broadband infrared light by the illuminator. ### Claim 10 (depends on 1) A projection data generation method for generating projection data of an object, the method comprising: providing the radiation for traversing the object by a radiation source; detecting the radiation, after having traversed the object; generating a detection signal depending on the detected radiation by the detector as defined in claim 1; and generating the projection data depending on the generated detection signal. ### Claim 11 (depends on 1) A detection computer program for detecting radiation, the detection computer program comprising program code means for causing a detector as defined in claim 1 to carry out the steps of the detection method, when the computer program is run on a computer controlling the detector. ### Claim 12 (depends on 8) A projection data generation computer program for generating projection data of an object, the computer program comprising program code means for causing a projection data generation system as defined in claim 8 to carry out the steps of the projection data generation method, when the computer program is run on a computer controlling the projection data generation system. ### Claim 13 (depends on 1) The detector as defined in claim 1, wherein the at least one band of the illumination light includes the broadband visible light wavelengths between 380 nm to 780 nm.