Methods and systems for establishing a kinetic model input function (IF) in positron emission tomography and single-photon emission computed tomography are provided. A position of interaction along a scintillating fiber coil is determined by: detecting a first plurality and second plurality of photons at first and second ends of the scintillating fiber coil; associating the first plurality of photons and the second plurality of photons with the interaction event based on a timing parameter; and determining a position of interaction for the interaction event based on a comparison between a first parameter of the first plurality of photons and a second parameter of the photons in the second plurality of photons.

An X-ray detector is provided. The X-ray detector includes multiple detector sub-modules. Each detector sub-module includes a semiconductor layer and multiple detector elements. A plurality of detector elements is disposed on the semiconductor layer. Wiring traces extending from the plurality of detector elements to readout circuitry, where each detector element is coupled to a respective wiring trace. One or more of the wiring traces extend over one or more detector elements of the plurality of detector elements. Processing circuitry is configured to perform coincidence detection to determine which detector element of the plurality of detector elements is associated with a location of an X-ray hit when the X-ray coincidently hits one of the detector elements of the plurality of detector elements and one or more of the wiring traces coupled to respective detector elements of the plurality of detector elements.

Disclosed herein are methods and devices for the acquisition of positron emission (or PET) data in the presence of ionizing radiation that causes afterglow of PET detectors. In one variation, the method comprises adjusting a coincidence trigger threshold of the PET detectors during a therapy session. In one variation, the method comprises adjusting a gain factor used in positron emission data acquisition (e.g., a gain factor used to multiply and/or shift the output(s) of a PET detector(s)) during a therapy session. In some variations, a method for acquiring positron emission data during a radiation therapy session comprises suspending communication between the PET detectors and a signal processor of a controller for a predetermined period of time after a radiation pulse has been emitted by the linac.

Disclosed herein are methods and devices for the acquisition of positron emission (or PET) data in the presence of ionizing radiation that causes afterglow of PET detectors. In one variation, the method comprises adjusting a coincidence trigger threshold of the PET detectors during a therapy session. In one variation, the method comprises adjusting a gain factor used in positron emission data acquisition (e.g., a gain factor used to multiply and/or shift the output(s) of a PET detector(s)) during a therapy session. In some variations, a method for acquiring positron emission data during a radiation therapy session comprises suspending communication between the PET detectors and a signal processor of a controller for a predetermined period of time after a radiation pulse has been emitted by the linac.

A radiation imaging apparatus includes a pixel array, a bias line, a plurality of drive lines, and a driving unit configured to cyclically supply an ON voltage to the drive lines. The radiation imaging apparatus also includes an acquiring unit configured to acquire a plurality of signal values by acquiring a signal value representing a current flowing through the bias line at each of a plurality of times within a period in which the ON voltage is continuously supplied to at least one of the plurality of drive lines, and a processing unit configured to specify an outlier in the plurality of signal values and determine whether or not there is a radiation irradiation with respect to the pixel array based on a signal value among the plurality of signal values that is not an outlier, and without being based on the outlier.

A radiation imaging apparatus includes a pixel array, a bias line, a plurality of drive lines, and a driving unit configured to cyclically supply an ON voltage to the drive lines. The radiation imaging apparatus also includes an acquiring unit configured to acquire a plurality of signal values by acquiring a signal value representing a current flowing through the bias line at each of a plurality of times within a period in which the ON voltage is continuously supplied to at least one of the plurality of drive lines, and a processing unit configured to specify an outlier in the plurality of signal values and determine whether or not there is a radiation irradiation with respect to the pixel array based on a signal value among the plurality of signal values that is not an outlier, and without being based on the outlier.

An X-ray detector is provided. The X-ray detector includes multiple detector sub-modules. Each detector sub-module includes a semiconductor layer and multiple detector elements. A first detector element of the multiple detector elements includes a first electrode disposed on a first doped implant and a second detector element of the multiple detector elements includes a second electrode disposed on a second doped implant. The first and second detector elements are disposed on the semiconductor layer adjacent to each other with a gap therebetween. Each detector sub-module also includes wiring traces extending from one or more detector elements of the multiple detector elements to readout circuitry. The wiring traces are routed within the gap between the first and second electrodes. The first doped implant extends underneath a portion of the wiring traces is configured to shield the wiring traces from electrical activity occurring underneath due to absorption of an X-ray.

An X-ray detector is provided. The X-ray detector includes multiple detector sub-modules. Each detector sub-module includes a semiconductor layer and multiple detector elements. A first detector element of the multiple detector elements includes a first electrode disposed on a first doped implant and a second detector element of the multiple detector elements includes a second electrode disposed on a second doped implant. The first and second detector elements are disposed on the semiconductor layer adjacent to each other with a gap therebetween. Each detector sub-module also includes wiring traces extending from one or more detector elements of the multiple detector elements to readout circuitry. The wiring traces are routed within the gap between the first and second electrodes. The first doped implant extends underneath a portion of the wiring traces is configured to shield the wiring traces from electrical activity occurring underneath due to absorption of an X-ray.

An X-ray detector is provided. The X-ray detector includes multiple detector sub-modules. Each detector sub-module includes a semiconductor layer and multiple detector elements. A first detector element of the multiple detector elements includes a first electrode disposed on a first doped implant and a second detector element of the multiple detector elements includes a second electrode disposed on a second doped implant. The first and second detector elements are disposed on the semiconductor layer adjacent to each other with a gap therebetween. Each detector sub-module also includes wiring traces extending from one or more detector elements of the multiple detector elements to readout circuitry. The wiring traces are routed within the gap between the first and second electrodes. The first doped implant extends underneath a portion of the wiring traces is configured to shield the wiring traces from electrical activity occurring underneath due to absorption of an X-ray.

Disclosed herein are methods and devices for the acquisition of positron emission (or PET) data in the presence of ionizing radiation that causes afterglow of PET detectors. In one variation, the method comprises adjusting a coincidence trigger threshold of the PET detectors during a therapy session. In one variation, the method comprises adjusting a gain factor used in positron emission data acquisition (e.g., a gain factor used to multiply and/or shift the output(s) of a PET detector(s)) during a therapy session. In some variations, a method for acquiring positron emission data during a radiation therapy session comprises suspending communication between the PET detectors and a signal processor of a controller for a predetermined period of time after a radiation pulse has been emitted by the linac.