# US 2014/0191136 A1 · Photon counting imaging method and device with instant retrigger capability > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2014/0191136 A1 - Document ID: US20140191136A1 - Status: Published application - Kind: A1 - Application number: 14/233,899 - Filed: 2012-07-19 - Published: 2014-07-10 - Earliest claimed: 2011-07-20 - Assignees: Dectris AG - Inventors: Teddy Loeliger; Christian Broennimann; Roger Schnyder - Web page: https://patentgrep.com/patent/US20140191136A1 ## CPC - G01T 1/171: {Compensation of dead-time counting losses} - 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) ## Abstract A method for photon counting imaging with improved high-rate counting performance includes the step of applying an instant retrigger capability with adjustable dead time in cells of the detector array and operates an apparatus using a layer of photo-sensitive material, an L×K array of photodetector elements arranged in the layer of the photosensitive material, an N×M array of readout unit cells, including amplifying elements and at least one readout unit cells for at least one photodetector elements. The readout unit cells are controlled by signal processing elements with each readout unit cell having internal signal processing elements to generate a discriminator output signal representing an amplified signal of the electron-hole pairs generated by an incident photon or a number of incident photons in the respective photodetector element. The discriminator output signal is generated by comparing the amplified signal with a predetermined threshold level and the discriminator output signal is generated whenever the amplified signal exceeds the threshold level. ## Claims ### Claim at position 1 1-15. (canceled) ### Claim 16 A method for photon counting imaging for single X-ray counting using a layer of photosensitive material, an L×K array photodetector elements arranged ni the layer of the photosensitive material, an N×M array of readout unit cells including amplifying elements, K, L, M and N being numbers greater than or equal to one, at least one readout unit cell for at least one photodetector element, said at least one readout unit cells being controlled via signal processing elements, each said readout unit cell comprising internal signal processing elements allowing to generate a discriminator output signal representing an amplified signal of electron-hole pairs generated by at least one an incident photon in said least one photodetector element, the discriminator output signal being generated by comparing the amplified signal with a predetermined threshold level and the discriminator output signal being generated whenever the amplified signal exceeds the predetermined threshold level with a counter unit registering counts as a function of the discriminator output signal, said method comprising the steps of: registering the counts by counting for each signal pulse a number of dead time intervals of a predetermined width corresponding to a width of the signal pulse at the discriminator output by starting a dead time interval whenever the amplified signal initially exceeds the predetermined threshold level; and, counting directly succeeding dead time intervals for as long as the amplified signal exceeds the predetermined threshold level. ### Claim 17 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, wherein said step of registering the counts is carried out with the count being registered and a dead time interval sequence is started whenever no dead time interval is currently running and the amplified signal is being reevaluated and, if the amplified signal exceeds the predetermined threshold level, said counting step is re-triggered and registers a new count, and generation of the dead time is started anew for further potential re-triggering, otherwise, if the amplified signal does not exceed the predetermined threshold level after termination of the dead time interval, then said counting is not re-triggered thereby registering no new count, and the dead time interval sequence is ended. ### Claim 18 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, further comprising the step of: generating a time stamp via a time piece for the discriminator output signal so generated. ### Claim 19 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, further comprising the step of: adjusting the dead time for each said readout unit cell. ### Claim 20 (depends on 19) The method for photon counting imaging for single X-ray counting according to claim 19, wherein the dead time is the same for each said readout unit cell. ### Claim 21 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, further comprising the step of: adjusting a same dead line overlap for each said readout unit cell with the dead time overlap being defined as dead-time-to-pulse-width ratio, or a ratio of width of the dead time to width of a nominal single photon pulse, the nominal single photon pulse being defined as a respective pulse generated by a single incident photon for effective processing parameter settings. ### Claim 22 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, further comprising the step of: activating or deactivating a plurality of operating modes via programming mode registers accessible as virtual readout unit cells. ### Claim 23 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, further comprising the step of: determining an incoming photon rate by multiplying a final counter value of each said readout unit cell from all countered discriminator output signal pulses with re-triggered counting during exposure time with a predetermined factor depending upon counter value for obtaining a count rate correction, said exposure time being a number corresponding to accumulated widths of all said discriminator output signal pulses including pile-up pulses. ### Claim 24 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, further comprising the step of: determining an incoming photon rate by multiplying individual counter values of each said readout unit cell, each resulting from only one discriminator output signal pulse with re-triggered counting, with an individual predetermined factor depending on counter value for obtaining an event-driven pulse signal evaluation and count rate correction, said re-triggering counting being a number corresponding to a width of a single said discriminator output signal pulse or pile-up pulse. ### Claim 25 (depends on 16) The method for photon counting imaging for single X-ray counting according to claim 16, wherein each said readout unit cell generates multiple individual discriminator output signals, each of said discriminator signals being generated by comparing the amplified signal with an individual predetermined threshold level, one counter unit per individual discriminator registering counts as a function of the individual discriminator output signal, counts being registered by counting the number of dead time intervals of an individual predetermined width by starting an individual dead time interval sequence whenever the amplified signal is initially exceeding the individual threshold level, and individually counting the number of directly succeeding individual dead time intervals for as long as the amplified signal is exceeding the individual threshold level. ### Claim 26 (depends on 25) The method for photon counting imaging for single X-ray counting according to claim 25, wherein resulting counter values of each said readout unit cell is determined by the sum of weighted individual counter values of the individual counters of a respective said readout unit cell, the weighted individual counter value being defined as the individual counter value multiplied by an individual predetermined factor. ### Claim 27 An apparatus for photon counting imaging for single X-ray counting, comprising: a layer of photosensitive material; an L×K array of photodetector elements arranged in said layer of photosensitive material; signal processing elements; an N×M array of readout until cells including amplifying elements, K, L, M and N being numbers greater than or equal to one, one or a plurality of readout unit cells for one or a plurality of photodetector elements, said readout unit cells being controlled by said signal processing elements, each said readout unit cell comprising internal signal processing elements allowing to generate a discriminator output signal representing an amplified signal of electron-hole pairs generated by an incident photo or a plurality of incident photons in a respective said photodetector element, said discriminator output signal being generated by comparing the amplified signal with a predetermined threshold level and the discriminator output signal being generated whenever the amplified signal is exceeding the predetermined threshold level; a counting unit registering counts as a function of the discriminator output signal; and, a counting circuit comprising a dead time generation circuit, the dead time having a predetermined width, starting of the dead time being enabled as a function of the discriminator output signal at an input of the dead time generation circuit whenever counting is triggered as a function of the discriminator output signal and delivering a delayed signal at the output of the dead time generation circuit that re-enables a counting process and that re-triggers counting after the dead time if the amplified signal still exceeds the predetermined threshold level. ### Claim 28 (depends on 27) The apparatus for photon counting imaging for single X-ray counting according to claim 27, wherein said dead time generation circuit comprises adjustable circuit element for adjusting the width of the dead time. ### Claim 29 (depends on 27) The apparatus for photon counting imaging for single X-ray counting according to claim 27, wherein said dead time generation circuit comprises tapped delay circuit elements for adjusting the width of the dead time. ### Claim 30 (depends on 29) The apparatus for photon counting imaging for single X-ray counting according to claim 29, wherein said tapped delay circuit elements are inverters. ### Claim 31 (depends on 27) The apparatus for photon counting imaging for single X-ray counting according to claim 27, wherein said dead time generation circuit comprises tapped delay lines for adjusting the width of the dead time. ### Claim 32 (depends on 27) The apparatus for photon counting imaging for single X-ray counting according to claim 27, further comprising multiplexing means for external measurement of the output signals of the discriminator or said dead time generator circuit of the individual readout unit cells for experimentally determining width of a nominal single photon pulse or the width of the deadtime, said nominal single photon pulse being defined as a respective pulse generated via a single incident photon for effective processing parameter settings.