image quality noise linearity cross-field uniformity image artifacts
TRANSCRIPT
NOISE IN CT
FLUCTUATION OF CT# BETWEEN POINTS IN THE IMAGE FOR A SCAN OF UNIFORM MATERIAL SUCH WATER.
NOISE CAN BE MEASURED BY SCANNING
A WATER PHANTOM AND COMPUTING THE MEAN AND STANDARD DEVIATION FOR FOR A REGION OF INTEREST.
(ROI)
THE NOISE LEVELS FOR CT SCANNERS VARY AND DEPEND ON: MAS SCAN TIME KVP SLICE THICKNESS OBJECT SIZE ALGORITHM
NOISE IN CT IS MAINLYMAINLY RELATED TO PHOTON FLUX ( # OF DETECTED
PHOTONS) MATRIX SIZE (PIXEL SIZE) SLICE THICKNESS ALGORITHM ELECTRONIC NOISE ( DETECTOR
ELECTRONICS) SCATTER RADIATION
CROSS-FIELD UNIFORMITY
THE UNIFORMITY OF CT # THROUGHOUT THE ENTIRE SCAN FIELD OF VIEW IS ONE INDICATION THAT CT SCANNER IS PERFORMANCE IS ACCEPTABLE.
IT REFERS TO THE VALUES OF THE PIXELS IN THE RECONSTRUCTED IMAGE
THEY SHOULD BE CONSTANT AT ANY POINT IN THE IMAGE OF PHANTOM
TYPES AND CAUSES OF ARTIFACTS STREAKS IMPROPER
SAMPLING OF DATA PARTIAL VOLUME
AVERAGING PATIENT MOTION METAL & BEAM
HARDENING NOISE SPIRAL SCANNING MECHANICAL
FAILURE
TYPES AND CAUSES OF ARTIFACTS SHADING PART. VOLUME AVG.
BEAM HARDENING SPIRAL SCANNING SCATTER OFF-FOCUS
RADIATION INCOMPLETE
PROJECTION
MOTION ARTIFACT- VOLUNTARY & INVOLUNTARYCORRECTION: IMMOBILIZATION PROPER EXPLANATION OF
PROCEDURE SHORT SCAN TIME MOTION REDUCTION
SOFTWARE (SHIMADZU –MAC)
I
BEAM HARDENING ARTIFACT-CUPPING ARTIFACT INCREASE IN THE MEAN ENERGY OF
THE X-RAY BEAM AS IT PASSES THROUGH THE PATIENT
IT CAN OCCUR WHEN RADIATION BEAMS HAVE DIFFERENT PATH LENGTHS
EQUIPMENT INDUCED ARTIFACTS
STREAK ARTIFACTS
MECHANICAL FAILURE POOR GANTRY RIGIDITY MECHANICAL ASSIGNMENT TUBE ROTOR WOBBLE POOR SAMPLING OF THE DETECTOR BAD DETECTOR-RING ARTIFACTS ( III GEN.) TUBE ARCING
CORRECTION OF ALIASING ARTIFACT INCREASE NUMBER OF VIEWS OR RAY
SAMPLES PER VIEW.
CONVOLUTION FILTER (SOFTWARE METHOD)