The present invention relates to differential phase-contrast imaging, in particular to a structure of a diffraction grating, e.g. an analyzer grating and a phase grating, for X-ray differential phase-contrast imaging. In order to make better use of the X-ray radiation passing the object, a diffraction grating (14) for X-ray differential phase-contrast imaging is provided with at least one portion (24) of a first sub-area (26) and at least one portion (28) of a second sub-area (30). The first sub-area comprises a grating structure (54) with a plurality of bars (34) and gaps (36) being arranged periodically with a first grating pitch P G (38), wherein the bars are arranged such that thy change the phase and/or amplitude of an X-ray radiation and wherein the gaps are X-ray transparent. The second sub-area is X-ray transparent and wherein the at least one portion of the second sub-area provides an X-ray 1 transparent aperture (40) in the grating. Portions of the first and second sub-areas are arranged in an alternating manner in at least one direction (42).

An X-ray projection of a region of examination and an associated X-ray parameter are received via an interface, the X-ray projection including X-ray intensities in a first pixel set. The X-ray parameter relates to at least one X-ray voltage from an X-ray source. Scattered radiation intensity is determined in a second pixel set, the second pixel set being a subset of the first pixel set. A first calculation of first exposure parameters in the second pixel set then occurs, each of the first exposure parameters in a pixel of the second pixel set being based on the X-ray intensity in the pixel and the scattered radiation intensity in the pixel. Furthermore, a second calculation of a scalar second exposure parameter occurs based on the first exposure parameters and an adjustment of the X-ray parameter is performed by comparing the scalar second exposure parameter with a reference value.

An X-ray projection of a region of examination and an associated X-ray parameter are received via an interface, the X-ray projection including X-ray intensities in a first pixel set. The X-ray parameter relates to at least one X-ray voltage from an X-ray source. Scattered radiation intensity is determined in a second pixel set, the second pixel set being a subset of the first pixel set. A first calculation of first exposure parameters in the second pixel set then occurs, each of the first exposure parameters in a pixel of the second pixel set being based on the X-ray intensity in the pixel and the scattered radiation intensity in the pixel. Furthermore, a second calculation of a scalar second exposure parameter occurs based on the first exposure parameters and an adjustment of the X-ray parameter is performed by comparing the scalar second exposure parameter with a reference value.

Apparatus and methods for therapy delivery are disclosed. In one embodiment, a therapy delivery system includes a plurality of movable components including a radiation therapy nozzle and a patient pod for holding a patient, a patient registration module for determining a desired position of at least one of the plurality of movable components, and a motion control module for coordinating the movement of the least one of the plurality of movable components from a current position to the desired position. The motion control module includes a path planning module for simulating at least one projected trajectory of movement of the least one of the plurality of moveable components from the current position to the desired position.

A scintillation material is longitudinally packaged in a circumferentially surrounding sheath, where the sheath has a lower index of refraction than the scintillation material, to form a scintillation optic or scintillation fiber optic. The scintillation material yields secondary photons upon passage of a charged particle beam, such as a positively charged residual particle beam having transmitted through a sample. The internally generated secondary photons within the sheath are guided to a detector element by the difference in index of refraction. Multiple scintillation optics are assembled to form a two-dimensional scintillation array coupled to a two-dimensional detector array, such as for use in determination of state of the residual charged particle beam, determination of an exit point of the particle beam from the sample, path of the treatment beam, and/or tomographic imaging.

A scintillation material is longitudinally packaged in a circumferentially surrounding sheath, where the sheath has a lower index of refraction than the scintillation material, to form a scintillation optic or scintillation fiber optic. The scintillation material yields secondary photons upon passage of a charged particle beam, such as a positively charged residual particle beam having transmitted through a sample. The internally generated secondary photons within the sheath are guided to a detector element by the difference in index of refraction. Multiple scintillation optics are assembled to form a two-dimensional scintillation array coupled to a two-dimensional detector array, such as for use in determination of state of the residual charged particle beam, determination of an exit point of the particle beam from the sample, path of the treatment beam, and/or tomographic imaging.

The present disclosure relates to a medical apparatus including a hadron therapy device directing an imaging hadron beam along a beam path. The beam path crosses a subject of interest including a plurality of tissues having upstream and downstream boundaries and a target tissue having a target spot. The apparatus further includes a magnetic resonance imaging device for acquiring magnetic resonance data within an imaging volume including a portion of the subject of interest including the target spot and at least the portion of the beam path between the upstream boundary and the target spot. The apparatus further includes a hadron radiography system (HRS) acquiring a signal generated by the imaging hadron beam and a controller for determining a water equivalent path length of the beam path between upstream and downstream boundaries based on at least the signal.

A gradient coil assembly for a magnetic resonance imaging device is disclosed. The gradient coil assembly comprises a cylindrical carrier with conductors forming three gradient coils associated with three orthogonal physical gradient axes. The cylindrical carrier comprises at least two radial through openings at different angular positions. At least one of the conductors runs through at least one area of the carrier located circumferentially between the through openings.

A method of performing a radiological biopsy and associated system includes scanning a living human subject with a CT scanner to locate coordinates of an area of potential pathology and then using the coordinates to direct synchrotron radiation to a location at, or proximat the coordinates to obtain a high-resolution image of the area of potential pathology. The CT scan is accomplished with a CT scanner such as a C-Arm, vertical or horizontal CT scanner. A synchrotron radiation source emits synchrotron radiation through the subject and is processed by a processing system. The method and system allow for concurrent or sequential scanning of the subject by the CT scanner and synchrotron radiation scanner. The resulting images provide histological resolution of areas of potential pathology.

The invention comprises a method and apparatus for aligning a charged particle beam path for treating a tumor of a patient, comprising: a cancer therapy system comprising the charged particle beam path sequentially passing: from an injector, through a synchrotron, along a beam transport line, and through a nozzle; a first two-dimensional detector configured to measure a beam state of positively charged particles; and an integrated intelligent system configured to classify the beam state into a set of beam shape factors, the integrated intelligent system configured to correct the beam shape through application of a condition-action rule: (1) adjusting a first voltage delivered to a first magnet positioned in the beam line prior to the first two-dimensional detector and (2) altering the beam shape through application of a second voltage to a second magnet position in the beam line adjacent to the first magnet.