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Effects of ray profile modeling on resolution recovery in clinical CT

Purpose: Iterative image reconstruction gains more and more interest in clinical routine, as it promises to reduce image noise (and thereby patient dose), to reduce artifacts, or to improve spatial resolution. However, among vendors and researchers, there is no consensus of how to best achieve these...

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Published in:Medical physics (Lancaster) 2014-02, Vol.41 (2), p.021907-n/a
Main Authors: Hofmann, Christian, Knaup, Michael, Kachelrieß, Marc
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Knaup, Michael
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description Purpose: Iterative image reconstruction gains more and more interest in clinical routine, as it promises to reduce image noise (and thereby patient dose), to reduce artifacts, or to improve spatial resolution. However, among vendors and researchers, there is no consensus of how to best achieve these goals. The authors are focusing on the aspect of geometric ray profile modeling, which is realized by some algorithms, while others model the ray as a straight line. The authors incorporate ray-modeling (RM) in nonregularized iterative reconstruction. That means, instead of using one simple single needle beam to represent the x-ray, the authors evaluate the double integral of attenuation path length over the finite source distribution and the finite detector element size in the numerical forward projection. Our investigations aim at analyzing the resolution recovery (RR) effects of RM. Resolution recovery means that frequencies can be recovered beyond the resolution limit of the imaging system. In order to evaluate, whether clinical CT images can benefit from modeling the geometrical properties of each x-ray, the authors performed a 2D simulation study of a clinical CT fan-beam geometry that includes the precise modeling of these geometrical properties. Methods: All simulations and reconstructions are performed in native fan-beam geometry. A water phantom with resolution bar patterns and a Forbild thorax phantom with circular resolution patterns representing calcifications in the heart region are simulated. An FBP reconstruction with a Ram–Lak kernel is used as a reference reconstruction. The FBP is compared to iterative reconstruction techniques with and without RM: An ordered subsets convex (OSC) algorithm without any RM (OSC), an OSC where the forward projection is modeled concerning the finite focal spot and detector size (OSC-RM) and an OSC with RM and with a matched forward and backprojection pair (OSC-T-RM, T for transpose). In all cases, noise was matched to be able to focus on comparing spatial resolution. The authors use two different simulation settings. Both are based on the geometry of a typical clinical CT system (0.7 mm detector element size at isocenter, 1024 projections per rotation). Setting one has an exaggerated source width of 5.0 mm. Setting two has a realistically small source width of 0.5 mm. The authors also investigate the transition from setting one to two. To quantify image quality, the authors analyze line profiles through the resol
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However, among vendors and researchers, there is no consensus of how to best achieve these goals. The authors are focusing on the aspect of geometric ray profile modeling, which is realized by some algorithms, while others model the ray as a straight line. The authors incorporate ray-modeling (RM) in nonregularized iterative reconstruction. That means, instead of using one simple single needle beam to represent the x-ray, the authors evaluate the double integral of attenuation path length over the finite source distribution and the finite detector element size in the numerical forward projection. Our investigations aim at analyzing the resolution recovery (RR) effects of RM. Resolution recovery means that frequencies can be recovered beyond the resolution limit of the imaging system. In order to evaluate, whether clinical CT images can benefit from modeling the geometrical properties of each x-ray, the authors performed a 2D simulation study of a clinical CT fan-beam geometry that includes the precise modeling of these geometrical properties. Methods: All simulations and reconstructions are performed in native fan-beam geometry. A water phantom with resolution bar patterns and a Forbild thorax phantom with circular resolution patterns representing calcifications in the heart region are simulated. An FBP reconstruction with a Ram–Lak kernel is used as a reference reconstruction. The FBP is compared to iterative reconstruction techniques with and without RM: An ordered subsets convex (OSC) algorithm without any RM (OSC), an OSC where the forward projection is modeled concerning the finite focal spot and detector size (OSC-RM) and an OSC with RM and with a matched forward and backprojection pair (OSC-T-RM, T for transpose). In all cases, noise was matched to be able to focus on comparing spatial resolution. The authors use two different simulation settings. Both are based on the geometry of a typical clinical CT system (0.7 mm detector element size at isocenter, 1024 projections per rotation). Setting one has an exaggerated source width of 5.0 mm. Setting two has a realistically small source width of 0.5 mm. The authors also investigate the transition from setting one to two. To quantify image quality, the authors analyze line profiles through the resolution patterns to define a contrast factor (CF) for contrast-resolution plots, and the authors compare the normalized cross-correlation (NCC) with respect to the ground truth of the circular resolution patterns. To independently analyze whether RM is of advantage, the authors implemented several iterative reconstruction algorithms: The statistical iterative reconstruction algorithm OSC, the ordered subsets simultaneous algebraic reconstruction technique (OSSART) and another statistical iterative reconstruction algorithm, denoted with ordered subsets maximum likelihood (OSML) algorithm. All algorithms were implemented both without RM (denoted as OSC, OSSART, and OSML) and with RM (denoted as OSC-RM, OSSART-RM, and OSML-RM). Results: For the unrealistic case of a 5.0 mm focal spot the CF can be improved by a factor of two due to RM: the 4.2 LP/cm bar pattern, which is the first bar pattern that cannot be resolved without RM, can be easily resolved with RM. For the realistic case of a 0.5 mm focus, all results show approximately the same CF. The NCC shows no significant dependency on RM when the source width is smaller than 2.0 mm (as in clinical CT). From 2.0 mm to 5.0 mm focal spot size increasing improvements can be observed with RM. Conclusions: Geometric RM in iterative reconstruction helps improving spatial resolution, if the ray cross-section is significantly larger than the ray sampling distance. In clinical CT, however, the ray is not much thicker than the distance between neighboring ray centers, as the focal spot size is small and detector crosstalk is negligible, due to reflective coatings between detector elements. 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However, among vendors and researchers, there is no consensus of how to best achieve these goals. The authors are focusing on the aspect of geometric ray profile modeling, which is realized by some algorithms, while others model the ray as a straight line. The authors incorporate ray-modeling (RM) in nonregularized iterative reconstruction. That means, instead of using one simple single needle beam to represent the x-ray, the authors evaluate the double integral of attenuation path length over the finite source distribution and the finite detector element size in the numerical forward projection. Our investigations aim at analyzing the resolution recovery (RR) effects of RM. Resolution recovery means that frequencies can be recovered beyond the resolution limit of the imaging system. In order to evaluate, whether clinical CT images can benefit from modeling the geometrical properties of each x-ray, the authors performed a 2D simulation study of a clinical CT fan-beam geometry that includes the precise modeling of these geometrical properties. Methods: All simulations and reconstructions are performed in native fan-beam geometry. A water phantom with resolution bar patterns and a Forbild thorax phantom with circular resolution patterns representing calcifications in the heart region are simulated. An FBP reconstruction with a Ram–Lak kernel is used as a reference reconstruction. The FBP is compared to iterative reconstruction techniques with and without RM: An ordered subsets convex (OSC) algorithm without any RM (OSC), an OSC where the forward projection is modeled concerning the finite focal spot and detector size (OSC-RM) and an OSC with RM and with a matched forward and backprojection pair (OSC-T-RM, T for transpose). In all cases, noise was matched to be able to focus on comparing spatial resolution. The authors use two different simulation settings. Both are based on the geometry of a typical clinical CT system (0.7 mm detector element size at isocenter, 1024 projections per rotation). Setting one has an exaggerated source width of 5.0 mm. Setting two has a realistically small source width of 0.5 mm. The authors also investigate the transition from setting one to two. To quantify image quality, the authors analyze line profiles through the resolution patterns to define a contrast factor (CF) for contrast-resolution plots, and the authors compare the normalized cross-correlation (NCC) with respect to the ground truth of the circular resolution patterns. To independently analyze whether RM is of advantage, the authors implemented several iterative reconstruction algorithms: The statistical iterative reconstruction algorithm OSC, the ordered subsets simultaneous algebraic reconstruction technique (OSSART) and another statistical iterative reconstruction algorithm, denoted with ordered subsets maximum likelihood (OSML) algorithm. All algorithms were implemented both without RM (denoted as OSC, OSSART, and OSML) and with RM (denoted as OSC-RM, OSSART-RM, and OSML-RM). Results: For the unrealistic case of a 5.0 mm focal spot the CF can be improved by a factor of two due to RM: the 4.2 LP/cm bar pattern, which is the first bar pattern that cannot be resolved without RM, can be easily resolved with RM. For the realistic case of a 0.5 mm focus, all results show approximately the same CF. The NCC shows no significant dependency on RM when the source width is smaller than 2.0 mm (as in clinical CT). From 2.0 mm to 5.0 mm focal spot size increasing improvements can be observed with RM. Conclusions: Geometric RM in iterative reconstruction helps improving spatial resolution, if the ray cross-section is significantly larger than the ray sampling distance. In clinical CT, however, the ray is not much thicker than the distance between neighboring ray centers, as the focal spot size is small and detector crosstalk is negligible, due to reflective coatings between detector elements. Therefore,RM appears not to be necessary in clinical CT to achieve resolution recovery.</description><subject>ALGORITHMS</subject><subject>APPROXIMATIONS</subject><subject>Artifacts and distortion</subject><subject>Biological material, e.g. blood, urine; Haemocytometers</subject><subject>cardiology</subject><subject>clinical‐CT</subject><subject>Computed tomography</subject><subject>Computerised tomographs</subject><subject>computerised tomography</subject><subject>COMPUTERIZED TOMOGRAPHY</subject><subject>Digital computing or data processing equipment or methods, specially adapted for specific applications</subject><subject>GEOMETRY</subject><subject>HEART</subject><subject>Humans</subject><subject>Image data processing or generation, in general</subject><subject>image denoising</subject><subject>Image enhancement or restoration, e.g. from bit‐mapped to bit‐mapped creating a similar image</subject><subject>IMAGE PROCESSING</subject><subject>Image Processing, Computer-Assisted - methods</subject><subject>image reconstruction</subject><subject>image resolution</subject><subject>image sampling</subject><subject>Image sensors</subject><subject>ITERATIVE METHODS</subject><subject>iterative reconstruction</subject><subject>maximum likelihood estimation</subject><subject>MAXIMUM-LIKELIHOOD FIT</subject><subject>Medical image contrast</subject><subject>Medical image noise</subject><subject>medical image processing</subject><subject>Medical image reconstruction</subject><subject>Medical imaging</subject><subject>Models, Theoretical</subject><subject>Noise</subject><subject>Numerical approximation and analysis</subject><subject>Particle beam detectors</subject><subject>PHANTOMS</subject><subject>Phantoms, Imaging</subject><subject>Radiography, Thoracic</subject><subject>RADIOLOGY AND NUCLEAR MEDICINE</subject><subject>ray‐modeling</subject><subject>Reconstruction</subject><subject>REFLECTIVE COATINGS</subject><subject>resolution recovery</subject><subject>set theory</subject><subject>SIMULATION</subject><subject>SPATIAL RESOLUTION</subject><subject>Tomography, X-Ray Computed - methods</subject><subject>X‐ray detectors</subject><issn>0094-2405</issn><issn>2473-4209</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLAzEYRYMoWh8L_4AE3Kgw9ctj0pmllPoARRd1HdL0G41MJzWZKv33pk4VQTQEkpCTS-4h5JBBnzFWnLO-LBTPGWyQHpcDkUkO5SbpAZQy4xLyHbIb4wsAKJHDNtnhMgeleNEjo1FVoW0j9RUNZknnwVeuRjrzU6xd80R9QwNGXy9a97m1_g3DkrqG2nTvrKnpcLxPtipTRzxYr3vk8XI0Hl5nt_dXN8OL28xKziDjCMAVWj5gMElTIAolmFBQoMmNLFWBhUCQpuKFzCVTVk3KMh0sF_lEiD1y3OX62DodrWvRPlvfNKmC5jwpSCNRJx2VyrwuMLZ65qLFujYN-kXUTJYlEwNZrgJPO9QGH2PASs-Dm5mw1Az0yq1meu02sUfr2MVkhtNv8ktmArIOeE8Gl38n6buHdeBZx6-KmJXf7zdvPvzg59PqP_j3Vz8AfhaaNA</recordid><startdate>201402</startdate><enddate>201402</enddate><creator>Hofmann, Christian</creator><creator>Knaup, Michael</creator><creator>Kachelrieß, Marc</creator><general>American Association of Physicists in Medicine</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>201402</creationdate><title>Effects of ray profile modeling on resolution recovery in clinical CT</title><author>Hofmann, Christian ; Knaup, Michael ; Kachelrieß, Marc</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4210-2e0026ec2710b10b3ee36313608ea5a4968e83e04af2845416c6b99f28c235b33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>ALGORITHMS</topic><topic>APPROXIMATIONS</topic><topic>Artifacts and distortion</topic><topic>Biological material, e.g. blood, urine; Haemocytometers</topic><topic>cardiology</topic><topic>clinical‐CT</topic><topic>Computed tomography</topic><topic>Computerised tomographs</topic><topic>computerised tomography</topic><topic>COMPUTERIZED TOMOGRAPHY</topic><topic>Digital computing or data processing equipment or methods, specially adapted for specific applications</topic><topic>GEOMETRY</topic><topic>HEART</topic><topic>Humans</topic><topic>Image data processing or generation, in general</topic><topic>image denoising</topic><topic>Image enhancement or restoration, e.g. from bit‐mapped to bit‐mapped creating a similar image</topic><topic>IMAGE PROCESSING</topic><topic>Image Processing, Computer-Assisted - methods</topic><topic>image reconstruction</topic><topic>image resolution</topic><topic>image sampling</topic><topic>Image sensors</topic><topic>ITERATIVE METHODS</topic><topic>iterative reconstruction</topic><topic>maximum likelihood estimation</topic><topic>MAXIMUM-LIKELIHOOD FIT</topic><topic>Medical image contrast</topic><topic>Medical image noise</topic><topic>medical image processing</topic><topic>Medical image reconstruction</topic><topic>Medical imaging</topic><topic>Models, Theoretical</topic><topic>Noise</topic><topic>Numerical approximation and analysis</topic><topic>Particle beam detectors</topic><topic>PHANTOMS</topic><topic>Phantoms, Imaging</topic><topic>Radiography, Thoracic</topic><topic>RADIOLOGY AND NUCLEAR MEDICINE</topic><topic>ray‐modeling</topic><topic>Reconstruction</topic><topic>REFLECTIVE COATINGS</topic><topic>resolution recovery</topic><topic>set theory</topic><topic>SIMULATION</topic><topic>SPATIAL RESOLUTION</topic><topic>Tomography, X-Ray Computed - methods</topic><topic>X‐ray detectors</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hofmann, Christian</creatorcontrib><creatorcontrib>Knaup, Michael</creatorcontrib><creatorcontrib>Kachelrieß, Marc</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Medical physics (Lancaster)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hofmann, Christian</au><au>Knaup, Michael</au><au>Kachelrieß, Marc</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effects of ray profile modeling on resolution recovery in clinical CT</atitle><jtitle>Medical physics (Lancaster)</jtitle><addtitle>Med Phys</addtitle><date>2014-02</date><risdate>2014</risdate><volume>41</volume><issue>2</issue><spage>021907</spage><epage>n/a</epage><pages>021907-n/a</pages><issn>0094-2405</issn><eissn>2473-4209</eissn><coden>MPHYA6</coden><abstract>Purpose: Iterative image reconstruction gains more and more interest in clinical routine, as it promises to reduce image noise (and thereby patient dose), to reduce artifacts, or to improve spatial resolution. However, among vendors and researchers, there is no consensus of how to best achieve these goals. The authors are focusing on the aspect of geometric ray profile modeling, which is realized by some algorithms, while others model the ray as a straight line. The authors incorporate ray-modeling (RM) in nonregularized iterative reconstruction. That means, instead of using one simple single needle beam to represent the x-ray, the authors evaluate the double integral of attenuation path length over the finite source distribution and the finite detector element size in the numerical forward projection. Our investigations aim at analyzing the resolution recovery (RR) effects of RM. Resolution recovery means that frequencies can be recovered beyond the resolution limit of the imaging system. In order to evaluate, whether clinical CT images can benefit from modeling the geometrical properties of each x-ray, the authors performed a 2D simulation study of a clinical CT fan-beam geometry that includes the precise modeling of these geometrical properties. Methods: All simulations and reconstructions are performed in native fan-beam geometry. A water phantom with resolution bar patterns and a Forbild thorax phantom with circular resolution patterns representing calcifications in the heart region are simulated. An FBP reconstruction with a Ram–Lak kernel is used as a reference reconstruction. The FBP is compared to iterative reconstruction techniques with and without RM: An ordered subsets convex (OSC) algorithm without any RM (OSC), an OSC where the forward projection is modeled concerning the finite focal spot and detector size (OSC-RM) and an OSC with RM and with a matched forward and backprojection pair (OSC-T-RM, T for transpose). In all cases, noise was matched to be able to focus on comparing spatial resolution. The authors use two different simulation settings. Both are based on the geometry of a typical clinical CT system (0.7 mm detector element size at isocenter, 1024 projections per rotation). Setting one has an exaggerated source width of 5.0 mm. Setting two has a realistically small source width of 0.5 mm. The authors also investigate the transition from setting one to two. To quantify image quality, the authors analyze line profiles through the resolution patterns to define a contrast factor (CF) for contrast-resolution plots, and the authors compare the normalized cross-correlation (NCC) with respect to the ground truth of the circular resolution patterns. To independently analyze whether RM is of advantage, the authors implemented several iterative reconstruction algorithms: The statistical iterative reconstruction algorithm OSC, the ordered subsets simultaneous algebraic reconstruction technique (OSSART) and another statistical iterative reconstruction algorithm, denoted with ordered subsets maximum likelihood (OSML) algorithm. All algorithms were implemented both without RM (denoted as OSC, OSSART, and OSML) and with RM (denoted as OSC-RM, OSSART-RM, and OSML-RM). Results: For the unrealistic case of a 5.0 mm focal spot the CF can be improved by a factor of two due to RM: the 4.2 LP/cm bar pattern, which is the first bar pattern that cannot be resolved without RM, can be easily resolved with RM. For the realistic case of a 0.5 mm focus, all results show approximately the same CF. The NCC shows no significant dependency on RM when the source width is smaller than 2.0 mm (as in clinical CT). From 2.0 mm to 5.0 mm focal spot size increasing improvements can be observed with RM. Conclusions: Geometric RM in iterative reconstruction helps improving spatial resolution, if the ray cross-section is significantly larger than the ray sampling distance. In clinical CT, however, the ray is not much thicker than the distance between neighboring ray centers, as the focal spot size is small and detector crosstalk is negligible, due to reflective coatings between detector elements. Therefore,RM appears not to be necessary in clinical CT to achieve resolution recovery.</abstract><cop>United States</cop><pub>American Association of Physicists in Medicine</pub><pmid>24506628</pmid><doi>10.1118/1.4862510</doi><tpages>14</tpages></addata></record>
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subjects ALGORITHMS
APPROXIMATIONS
Artifacts and distortion
Biological material, e.g. blood, urine
Haemocytometers
cardiology
clinical‐CT
Computed tomography
Computerised tomographs
computerised tomography
COMPUTERIZED TOMOGRAPHY
Digital computing or data processing equipment or methods, specially adapted for specific applications
GEOMETRY
HEART
Humans
Image data processing or generation, in general
image denoising
Image enhancement or restoration, e.g. from bit‐mapped to bit‐mapped creating a similar image
IMAGE PROCESSING
Image Processing, Computer-Assisted - methods
image reconstruction
image resolution
image sampling
Image sensors
ITERATIVE METHODS
iterative reconstruction
maximum likelihood estimation
MAXIMUM-LIKELIHOOD FIT
Medical image contrast
Medical image noise
medical image processing
Medical image reconstruction
Medical imaging
Models, Theoretical
Noise
Numerical approximation and analysis
Particle beam detectors
PHANTOMS
Phantoms, Imaging
Radiography, Thoracic
RADIOLOGY AND NUCLEAR MEDICINE
ray‐modeling
Reconstruction
REFLECTIVE COATINGS
resolution recovery
set theory
SIMULATION
SPATIAL RESOLUTION
Tomography, X-Ray Computed - methods
X‐ray detectors
title Effects of ray profile modeling on resolution recovery in clinical CT
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