Optimization of the source firing pattern for X-ray scanning systems
US-9046465-B2 · Jun 2, 2015 · US
US9726619B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9726619-B2 |
| Application number | US-201514688898-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 16, 2015 |
| Priority date | Oct 25, 2005 |
| Publication date | Aug 8, 2017 |
| Grant date | Aug 8, 2017 |
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The present application discloses a computed tomography system having non-rotating X-ray sources that are programmed to optimize the source firing pattern. In one embodiment, the CT system is a fast cone-beam CT scanner which uses a fixed ring of multiple sources and fixed rings of detectors in an offset geometry. It should be appreciated that the source firing pattern is effectuated by a controller, which implements methods to determine a source firing pattern that are adapted to geometries where the X-ray sources and detector geometry are offset.
Opening claim text (preview).
We claim: 1. An X-ray imaging apparatus for obtaining a radiation image of an object having a length, comprising: N number of X-ray sources; and a controller in communication with each of said N number of X-ray sources, wherein the controller is programmed to cause each of said N number of X-ray sources to activate in a sequence, wherein said sequence is programmatically defined by a relationship: φ( i )=( k ( i− 1)mod N s )+1 wherein the controller is programmed to model said X-ray sources as being distributed around a surface of a cylinder in a form of a uniform distribution of triangles, wherein k is equal to an increment between X-ray sources being activated and is selected to make said triangles as equilateral as possible, and wherein i is equal to a projection number. 2. The X-ray imaging apparatus of claim 1 wherein the sequence of X-ray source activation creates a trajectory and wherein the trajectory is helical. 3. The X-ray imaging apparatus of claim 1 wherein said sequence of X-ray source activation is dynamically modulated based upon image data obtained from a prior scan. 4. The X-ray imaging apparatus of claim 1 wherein the sequence of X-ray source activation creates a trajectory and wherein the trajectory is non-helical. 5. The X-ray imaging apparatus of claim 4 wherein k is not equal to 1. 6. The X-ray imaging apparatus of claim 1 wherein said sequence of X-ray source activation is selected to obtain an even distribution of X-ray angles intersecting each voxel of a reconstruction volume over a range of 360 degrees over a length of the object. 7. The X-ray imaging apparatus of claim 1 wherein k is defined at least in part by using a relation: l 1 2 = d 2 + ( k - 1 p z N s ) 2 wherein d is a distance between adjacent sources, p z is a measure of pitch z, k −1 is an inverse of k modulo Ns and l 1 is a length of a side of a triangle. 8. The X-ray imaging apparatus of claim 1 wherein k is defined at least in part by using a relation: l 2 2 = ( 2 d ) 2 + p z 2 ( 2 k - 1 N s - 1 ) 2 wherein d is a distance between adjacent sources, p z is a measure of pitch z, k −1 is an inverse of k modulo Ns and l 2 is a length of a side of a triangle. 9. The X-ray imaging apparatus of claim 1 wherein k is defined at least in part by using a relation: l 3 2 = d 2 + p z 2 ( 1 - k - 1 N s ) 2 wherein d is a distance between adjacent sources, p z is a measure of pitch z, k −1 is an inverse of k modulo Ns and l 3 is a length of a side of a triangle. 10. The X-ray imaging apparatus of claim 1 wherein the X-ray sources are stationary. 11. The X-ray imaging apparatus of claim 10 wherein the X-ray sources have a rotationally invariant activation sequence. 12. The X-ray imaging apparatus of claim 1 wherein a configuration of the X-ray sources and a plurality of detectors has multi-fold symmetry. 13. The X-ray imaging apparatus of claim 12 wherein said configuration of the X-ray sources and the plurality of detectors exhibit 24 fold symmetry. 14. The X-ray imaging apparatus of claim 1 wherein said controller selects the sequence of X-ray source activation in order to create an evenly spaced sampling lattice over a surface of a virtual cylinder. 15. The X-ray imaging apparatus of claim 14 wherein a length of the virtual cylinder is equal to the length of the object plus a distance, wherein said distance is within a range of 0 mm to 100 mm. 16. The X-ray imaging apparatus of claim 1 further comprising a plurality of sensors arranged in a ring around the object for detecting X-rays emitted from the X-ray sources after passing through the object, wherein the sensors are offset from the X-ray sources along a predefined axis.
Cone-beams · CPC title
characterised by using a plurality of source units · CPC title
using tomography, e.g. computed tomography [CT] · CPC title
Control of apparatus or devices for radiation diagnosis · CPC title
using a detector unit almost surrounding the patient, e.g. more than 180° · CPC title
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