Provided are an X-ray imaging panel capable of suppressing a leak current of a photoelectric conversion layer while reducing the number of steps for manufacturing the imaging panel, and a method for manufacturing the same. An imaging panel 1 generates an image based on scintillation light obtained from X-rays passing through a subject. The imaging panel 1 is provided with a thin film transistor 13, passivation films 103 and 104 covering the thin film transistor 13, a photoelectric conversion layer 15 converting scintillation light into a charge, an upper electrode 16, and a lower electrode 14 connected to the thin film transistor 13, on a substrate 101. End portions of the lower electrode 14 are disposed on an inner side than the end portions of the photoelectric conversion layer 15. The lower electrode 14 and the thin film transistor 13 are connected to each other via a contact hole CH1 formed in the passivation films 103 and 104, in a region in which the photoelectric conversion layer 15 is provided.

A radiation detector including: a substrate formed with plural pixels that accumulate electrical charges generated in response to light converted from radiation in a pixel region at an opposite-side surface of a base member to a surface including a fine particle layer; the base member being flexible and is made of resin and that includes a fine particle layer containing inorganic fine particles having a mean particle size of from 0.05 μm to 2.5 μm, a conversion layer provided at the surface of the base member provided with the pixel region and configured to convert the radiation into light; and a reinforcement substrate provided to at least one out of a surface on the substrate side of a stacked body configured by stacking the substrate and the conversion layer, or a surface on the conversion layer side of the stacked body.

A data processing apparatus according to an embodiment includes acquisition circuitry and specification circuitry. The acquisition circuitry is configured to acquire a detector signal containing a first component that is based on Cherenkov light and a second component that is based on scintillation light. The specification circuitry is configured to specify timing information about generation of the detector signal by curve fitting to the first component.

An active matrix substrate includes a photoelectric conversion element 12, a first planarizing film 107, a first inorganic insulating film 108a, and a bias wire 16. The first planarizing film 107 covers the photoelectric conversion element 12 and has a first opening 107h at a position at which the first opening 107h overlaps with the photoelectric conversion element 12 in plan view. The first inorganic insulating film 108a has a second opening on an inner side of the first opening h and covers a surface of the first planarizing film 107. The bias wire 16 is provided on a first inorganic insulating film 108a and is connected to the photoelectric conversion element 12 via the second opening CH2.

According to one embodiment, a sensitivity correction method includes acquiring count rates for respective pixels in a photon counting detector; preparing incident dose adjustment materials for the respective pixels based on the count rates for the respective pixels; and providing the incident dose adjustment materials in a surface of the photon counting detector.

A photodetecting device is provided. The photodetecting device includes an array substrate. The first scan line extends in a first direction. The first data line extends in a second direction, wherein first data line is crossed with the first scan line. The first electronic unit is electrically connected to the first scan line and the first data line. The second electronic unit is adjacent to the first electronic unit and is disposed along the first direction. The third electronic unit is adjacent to the first electronic unit and is disposed along the second direction. The common line transmits a signal to the first electronic unit, the second electronic unit and the third electronic unit. The common line is disposed between the first electronic unit and the second electronic unit, or between the first electronic unit and the third electronic unit.

A radiation detection system that includes a radiation detector, a photo multiplier tube, and a pulse height analyzer. The radiation detector is configured to emit light when exposed to radiation. The photo multiplier tube is configured to convert the light to an electrical signal. The pulse height analyzer is configured to output at least one value associated with an amount of radiation detected based on at least in part on the electrical signal.

The disclosure provides a light detection device and a detection method for controlling a light source device. The light detection device includes a detection panel and a processor. The detection panel converts an input light from the light source device into a converted light and converts the converted light into a charge. The processor selects a first region and a second region other than the first region from the detection panel. A first charge of the converted light received by at least one first pixel of the first region during a first period is used to detect a dose of the input light. A second charge of the converted light received by the second region during the first period is used to generate a data image. The charge of the converted light received by at least one first pixel during a second period is used to generate the data image.

The present invention relates to a detection device for X-rays, an imaging system and a method for detecting electro-magnetic radiation using a detection device for X-rays, wherein an estimate of an incomplete measurement is acquired prior to a discontinuity of the electromagnetic radiation, wherein the discontinuity is a change or interruption in a beam or in an intensity of the electromagnetic radiation.

A method is provided for determining the dose rate {dot over (H)} of nuclear radiation field, namely a gamma radiation field, with a radiation detection system (RDS), comprising a scintillator, a photodetector, an amplifier and a pulse measurement electronics. The pulse measurement electronics includes a sampling analog to digital converter, where the nuclear radiation deposes at least some of its energy in the scintillator, thereby producing excited states in the scintillation material, with the excited states decaying thereafter under emission of photons with a decay time . Photons are absorbed by the photodetector under emission of electrons, those electrons forming a current pulse, said current pulse being amplified so that the resulting current signal can be processed further in order to determine the charge of the pulse measured.