US2018021002A1PendingUtilityA1

Scatter estimation and/or correction in x-ray imaging

Assignee: PRISMATIC SENSORS ABPriority: Jun 26, 2015Filed: Sep 29, 2017Published: Jan 25, 2018
Est. expiryJun 26, 2035(~8.9 yrs left)· nominal 20-yr term from priority
A61B 6/4291A61B 6/032A61B 6/4241A61B 6/5282A61B 6/4266G01T 1/2985A61B 6/4233
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Claims

Abstract

Disclosed are methods and devices for estimating object scatter and/or internal scatter in a multi-level photon-counting x-ray detector, as well as x-ray tomographic imaging while correcting for object and internal scatter. The x-ray detector has at least two layers of detector diodes mounted in an edge-on geometry, e.g. designed for 1) estimating the object scatter contribution to the counts in a top layer of the at least two layers based on difference(s) in counts between the top layer and lower layer(s) under the assumption the object scatter has a slowly varying spatial distribution, and/or 2) estimating counts from reabsorption of photons that have Compton scattered inside the detector based on selectively blinding some detector elements from primary radiation by placing a highly attenuating beam stop on top of the detector elements, in lower layer(s) or in both top layer and lower layer(s), and measuring the counts in those detector elements.

Claims

exact text as granted — not AI-modified
1 . A method for estimating internal scatter of a photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays,
 the method comprising estimating counts from reabsorption of photons that have Compton scattered inside the detector based on selectively blinding some detector elements from primary radiation by placing a highly attenuating beam stop on top of the detector elements, in lower layer(s) or in both top layer and lower layer(s), and measuring the counts in those detector elements.   
     
     
         2 . The method of  claim 1 , wherein the estimation is performed for each of a number of projections during rotation of a gantry of a computed tomography system. 
     
     
         3 . The method of  claim 1 , wherein the x-ray detector is a direct conversion x-ray detector using a direct-converter material. 
     
     
         4 . A method for adjusting measured counts in a layered photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays,
 the method comprising adjusting the measured counts at least partly based on the internal scatter estimated according to  claim 1 , to thereby obtain unbiased estimates of the counts due to primary x-ray interactions.   
     
     
         5 . A method for estimating the total amount and spatial profile of scattered radiation absorbed in a layered photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays,
 the method comprising performing the estimation at least partly based on the internal scatter estimated according to  claim 1 .   
     
     
         6 . A method for x-ray tomographic imaging of an object while correcting for scatter, wherein said method comprises:
 providing a source of x-ray radiation and detector comprising two layers of direct conversion semiconductor diodes pointing back to the source, wherein a spacing between individual diodes is provided in both a top and bottom layer that corresponds to the diode width, and a displacement of the bottom layer in the rotational direction such that primary x-rays missing the top layer diodes pass unattenuated to the lower level diodes;   providing beam stops, covering less than 50% of all detector channels and distributed across the entire detector, in the bottom layer or both the top and bottom layers, making them essentially blind to primary unscattered x-rays;   moving the source and detector around the object obtaining projection x-ray images at different rotation angles;   detecting radiation from the source by the detector;   estimating, for each rotation angle, the distribution of the sum of object and internal scatter of each layer by fitting a parametric surface to the counts of the detector elements with beam stops mounted on top of them; and   subtracting the estimated sum of object and internal scatter from each detector element not covered with beam stops, thus obtaining an estimate of the scatter free signal of each detector element not covered with beam stops.   
     
     
         7 . A device for estimating internal scatter of a photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays,
 wherein said device is configured to estimate counts from reabsorption of photons that have Compton scattered inside the detector based on measuring counts in detector elements having a highly attenuating beam stop placed on top of the detector elements, in lower layer(s) or in both top layer and lower layer(s).   
     
     
         8 . A device for adjusting measured counts in a layered photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays, wherein said device comprises a device of  claim 7 . 
     
     
         9 . A device for estimating the total amount and spatial profile of scattered radiation absorbed in a layered photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays, wherein said device comprises a device of  claim 7 . 
     
     
         10 . A device for x-ray tomographic imaging of an object while correcting for scatter, wherein said device comprises:
 a source of x-ray radiation and detector comprising two layers of direct conversion semiconductor diodes pointing back to the source,   wherein there is a spacing between individual diodes in both a top and bottom layer that corresponds to the diode width, and a displacement of the bottom layer in the rotational direction such that primary x-rays missing the top layer diodes pass unattenuated to the lower level diodes,   wherein beam stops are provided, covering less than 50% of all detector channels and distributed across the entire detector, in the bottom layer or both the top and bottom layers, making them essentially blind to primary unscattered x-rays;   wherein the source and detector are arranged to be moved around the object obtaining projection x-ray images at different rotation angles, controlled by a movement controller; and   an estimator, connected to the detector and arranged for obtaining measurement data from the detector, or being an integrated part of the detector, wherein the estimator is configured for estimating, for each rotation angle, the distribution of the sum of object and internal scatter of each layer by fitting a parametric surface to the counts of the detector elements with beam stops mounted on top of them, and the estimated sum of object and internal scatter is subtracted from each detector element not covered with beam stops, thus obtaining an estimate of the scatter free signal of each detector element not covered with beam stops.   
     
     
         11 . A non-transitory computer-readable medium having stored thereon a computer program for estimating, when executed by a processor, internal scatter of a photon-counting x-ray detector having at least two layers of detector diodes mounted in an edge-on geometry or at least two layers of diode segments of diodes segmented in the direction of the incoming x-rays,
 wherein said computer program comprises instructions, which when executed by the processor, cause the processor to estimate counts from reabsorption of photons that have Compton scattered inside the detector based on measurements of counts in detector elements having a highly attenuating beam stop placed on top of the detector elements, in lower layer(s) or in both top layer and lower layer(s).

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