CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

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CT and IGCT CT and IGCT Norbert J. Pelc, Sc.D. Norbert J. Pelc, Sc.D. Department of Radiology Department of Radiology Stanford University Stanford University
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Transcript of CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Page 1: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

CT and IGCTCT and IGCT

Norbert J. Pelc, Sc.D.Norbert J. Pelc, Sc.D.Department of RadiologyDepartment of Radiology

Stanford UniversityStanford University

Page 2: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

OutlineOutline

• We get the best toysWe get the best toysopportunities in MDCTopportunities in MDCT

• And we make some toys tooAnd we make some toys tooInverse Geometry CT (IGCT)Inverse Geometry CT (IGCT)

Page 3: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

CT Input/Output

array of projection

data

CTReconstruction

Program

distributionof

Page 4: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Filtered-backprojectionFiltered-backprojection

QuickTime™ and aCinepak decompressor

are needed to see this picture.

Page 5: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Volumetric coverageVolumetric coverage

Multi-slice helicalMulti-slice helicalrequires fewer rotationsrequires fewer rotations

source

detector

*

Helical CTHelical CTrequires multiple rotationsrequires multiple rotations

source

detector

*

Page 6: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.
Page 7: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

The Continuing Evolution: MDCTThe Continuing Evolution: MDCT

ManufacturerManufacturergantry gantry

rotationrotationdetector detector

rowsrowselectronics electronics

rowsrowsslicesslices

GEGE(Lightspeed VCT)(Lightspeed VCT)

0.35 s0.35 s 64 x 0.62564 x 0.625 6464 64/40mm64/40mm

PhilipsPhilips((Brilliance CT 64))

0.4 s0.4 s 64 x 0.62564 x 0.625 6464 64/40 mm64/40 mm

SiemensSiemens(Sensation 64)(Sensation 64)

0.33 s0.33 s32 x 0.632 x 0.6+ 8 x 1.2+ 8 x 1.2

323264/20 mm64/20 mm24/32 mm24/32 mm

ToshibaToshiba(Aquilion 64)(Aquilion 64)

0.4 s0.4 s 64 x 0.564 x 0.5 6464 64/32 mm64/32 mm

Page 8: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

CT future directionsCT future directions

• CheaperCheaperlower cost multi-row detectors and electronicslower cost multi-row detectors and electronicslower cost computer systemslower cost computer systems

• FasterFasterscan times < 100 msscan times < 100 ms

• BetterBetter QuickTime™ and aCinepak decompressor

are needed to see this picture.

Page 9: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Multi-source systemsMulti-source systems

Berninger et al, US Patent 4,196,352, filed 1978

• reduced minimum gantry rotation

• significant increase in scan speed and cost

• could have major application impact

Page 10: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

CT future directionsCT future directions

• CheaperCheaperlower cost multi-row detectors and electronicslower cost multi-row detectors and electronicslower cost computer systemslower cost computer systems

• FasterFasterscan times < 100 msscan times < 100 msfaster volumetric coveragefaster volumetric coverage “ “an organ in a rotation”an organ in a rotation”

• BetterBetter

Page 11: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

CT future directionsCT future directions

• CheaperCheaperlower cost multi-row detectors and electronicslower cost multi-row detectors and electronicslower cost computer systemslower cost computer systems

• FasterFasterscan times < 100 msscan times < 100 msfaster volumetric coveragefaster volumetric coverage “ “an organ in a rotation”an organ in a rotation”

• BetterBetterbetter contrast discriminationbetter contrast discriminationhigher spatial resolutionhigher spatial resolutionlower doselower dose

Page 12: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

CT future directionsCT future directions

• CheaperCheaperlower cost multi-row detectors and electronicslower cost multi-row detectors and electronicslower cost computer systemslower cost computer systems

• FasterFasterscan times < 100 msscan times < 100 msfaster volumetric coveragefaster volumetric coverage “ “an organ in a rotation”an organ in a rotation”

• BetterBetterbetter contrast discriminationbetter contrast discriminationhigher spatial resolutionhigher spatial resolutionlower doselower dose

Page 13: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Volumetric CT approachesVolumetric CT approaches

Multi-row helicalMulti-row helicalrequires multiple rotationsrequires multiple rotations

source

detector

*

*source

detector

Cone beam VCTCone beam VCT

Scan the volume in a single rotation, or step-and-shoot

Page 14: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

VCT with flat panel detectorsVCT with flat panel detectors

GE CR&DGE CR&D

Siemens Axiom ArtisSiemens Axiom Artis

Page 15: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Cone beam artifactsCone beam artifacts

Cone beam VCT system, stack of 9 disks9 cone angle (10 cm z-FOV @ 65 cm), Feldkamp reconstruction

K. Sourbelle, et al, , RSNA 2003, #183

Page 16: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Cone beam artifactsCone beam artifacts

Page 17: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Cone beam artifactsCone beam artifacts

indistingushableindistingushableobjectsobjects

fundamental problem, no correction exists

Page 18: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

2D scanned anode x-ray source

detector array

source and detector have the same axial extent

Inverse-Geometry CT (IGCT)Inverse-Geometry CT (IGCT)

• system designs

• reconstruction methods

• simulations and experiments

NexRay, Inc., Los Gatos, CA

detector array

Page 19: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Inverse-Geometry VCTInverse-Geometry VCT

AxialAxial SagittalSagittal

Page 20: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

““Defrise” phantomDefrise” phantom

No cone-beam artifacts!No cone-beam artifacts!

Cone-beam VCTCone-beam VCT IGCTIGCT

Page 21: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

Cadaver inner earCadaver inner ear

conventional IGCT

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 22: CT and IGCT Norbert J. Pelc, Sc.D. Department of Radiology Stanford University.

ConclusionsConclusions

• MDCTMDCTcheaper, faster, bettercheaper, faster, better

better spatial and temporal resolutionbetter spatial and temporal resolutionlower radiation doselower radiation dose

• ““Organ in a rotation” with outstanding Organ in a rotation” with outstanding image quality needs a different approachimage quality needs a different approach

Cannot use a simple point x-ray sourceCannot use a simple point x-ray sourceInverse Geometry CT (IGCT)Inverse Geometry CT (IGCT)

preliminary results are promisingpreliminary results are promising

• Hang on to your hat, the data will fly in!Hang on to your hat, the data will fly in!