Institute of Nuclear Energy Research, Atomic Energy Council, Executive Yuan, R.o.c

Institute of Nuclear Energy Research, Atomic Energy Council, Executive Yuan

Sheng-Pin Tseng

Meei-Ling Jan

Chia-Hao Chang

Yu-Ching Ni

Ho-Hui Hsieh

Fan-Pin Tseng

Chung-Hung Chang

Syuan-Ya Huang

Ming-Lee Chu

A calculation method for a dual-energy X-ray imaging system is provided. The calculation method for the dual-energy X-ray imaging system includes the following steps. A plurality of material attenuation coefficient ratio of the dual-energy projection image are established according to the reference materials with known material characteristics. The effective atomic number of each reference material and the material attenuation coefficient ratio are used to establish a calibration data set. A rational polynomial approximation method is adopted to obtain the characteristic model related to the material attenuation coefficient ratio of the reference material and the effective atomic number of the reference material. The material attenuation coefficient ratio of the dual-energy projection image of unknown material is established. The material attenuation coefficient ratio of the unknown material is substitute into the characteristic model to obtain the effective atomic number corresponding to the unknown material.

Calculation method for a dual-energy X-ray imaging system

A geometric calibration method for dual-axis digital tomosynthesis includes the steps of: providing a calibration phantom having a first plate, a second plate parallel to the first plate, and mark points distributed to the first and second plates; arranging any mark point at the first plate not to be vertically collinear with a mark point at the second plate; projecting the calibration phantom onto a planar detector to obtain a projected calibration-phantom image; deriving a conversion relationship between the mark point and the corresponding projected position at the planar detector to further establish a projection matrix related to an imaging system; and, applying the projection matrix to calculate a plurality of geometric parameters. In addition, a geometric calibration system for dual-axis digital tomosynthesis is also provided.

Geometric calibration method and system for dual axis digital tomosynthesis

The invention provides an automatic exposure control method for a digital X-ray imaging device. The automatic exposure control method for a digital X-ray imaging device includes the following the steps. First, a parameter database is provided before imaging scan. A depth information is generated, wherein the depth information by a depth sensor detect the thickness of a region of interest of an object. Imaging exposure parameters, mAs and kV, are estimated according to the depth information and the parameter database. Then, X-ray imaging is performed according to the imaging exposure parameters estimated by the method described in this application. In addition, an automatic exposure control system for a digital X-ray imaging device is also provided.

Automatic exposure control system for a digital X-ray imaging device and method thereof

A scanning system includes a first base, a bed panel, a bed board, a second base and an X-ray mechanism. The bed panel, movably located on the first base, includes a first image-receiving module. The bed board is movably located on the bed panel. The second base, located aside to the first base, includes a second image-receiving module. The X-ray mechanism, connected with the first base, includes an X-ray tube. While the bed panel and the bed board are moved away from the second base, and the X-ray mechanism is moved toward the second base; then, the X-ray tube would undergo a vertical movement to a position aside to a lateral side of the first base by facing the second base.

Scanning system

The invention provides a loading mechanism for x-ray tube. The loading mechanism for x-ray tube includes an x-ray tube, a swing element and a rotating element. The x-ray tube includes a focal spot location and an x-ray opening. The swing element includes a first rotating axis, and the first rotating axis passes through the focal spot location. The swing element rotates about the first axis to rotate the x-ray tube within a limit swing range. The rotating element is connected to the swing element. The rotating element has a second rotating axis, and the first rotating axis perpendicular to the second rotating axis. The rotating element rotates about the second rotating axis to drive rotate the x-ray tube and the swing element. In addition, the scanning system for three-dimensional image is provided.

Loading mechanism for x-ray tube and scanning system for three-dimensional imaging

A scanning system for three-dimensional imaging comprises a bench, a gantry frame, a light source, a sensor and a control unit. The bench is to support a subject to be scanned. The gantry frame is movably mounted at a lateral side of the bench. The light source is movably mounted on the gantry frame so as to emit a light for a radiographic purpose. The sensor is movably mounted at a side of the bench, by opposing to the subject with respect to the bench, so as to receive the light emitted from the light source. The control unit is electrically coupled with the gantry frame, the light source and the sensor so as thereby to perform motion controls upon the gantry frame, the light source and the sensor.

Scanning system for three-dimensional imaging

The invention relates to a method for radiation detection signal processing, and more particularly to a method capable of using a periodic signal to control the time of charging/discharging to a capacitor of an integrator. The method can be used for detecting the energy of incident photon of Gamma ray during the happening of an event while reducing dead time, and thereby, the count rate is increased. As the periodic signal is used as the signal for controlling the time of charging/discharging to a capacitor, the charging/discharging time of the integrator is no longer being controlled by the triggering time of the event, and thus, the present method is advantageous in that: the control method and circuit architecture are comparatively simpler since the charging/discharging time of the integrator no longer required to be controlled precisely, and thus the integration error due to insufficient resolution in delay element can be avoided.

Method for radiation detection signal processing

A radiation detection signal processing method and a radiation detection signal processing system using the method are provided, which combine trigger signals and time mark information. The method includes: providing a radiation detection signal processing system having a plurality of front-end detectors, where each front-end detector detects a radiation event to generate a corresponding energy signal; generating a corresponding trigger signal according to the corresponding energy signal; generating a first signal and a second signal according to all trigger signals; and obtaining time differences among the trigger signals according to the first signal and the second signal, converting the time differences into a set of time marks, merging all of the trigger signals and the set of time marks into a hybrid time signal, and transmitting the hybrid time signal to a hybrid event coincidence detection circuit.

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Taoyuan, Taiwan

Sheng-Pin Tseng