Radiography: 2D and 3D Metrics of Performance Towards Quality Index

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AAPM COMP 011 Radiography: D and 3D Metrics of Performance Towards Quality Index Ehsan Samei, Sam Richard Duke University Learning objectives Outlook 1. To understand methods for D and 3D resolution measurements.. To understand the basics for DQE and edqe measurement techniques. 3. To relate physical metrics of performance to clinical image quality. Medical imaging clinically meaningful information Quality of information image quality Image quality universally-appreciated universally-illusive 3 4 1 1

What is image quality? Image esthetics Subjective and qualitative Not necessarily reflective of diagnostic performance Diagnostic accuracy Expensive Impractical given the extent and variability of technologies Physical metrics of image quality Convenient and practical Effective to the extent they can be related to diagnostic performance Applicable under qualified conditions: Detector vs system Incorporation of scattered radiation Incorporation of anatomical attributes Incorporation of task attributes System-based vs image-based metrics Resolution Ability to resolve distinct features of an image from each other Resolution Best characterized by the modulation transfer function (MTF): The efficiency of an imaging system in reproducing subject contrast at various spatial frequencies MTF F{LSF(x)} Low resolution High resolution 7 8

High MTF Low MTF 9 10 Noise Unwanted signals that interfere with interpretation Noise Best characterized by the noise power spectrum (NPS): The variance of noise in an image in terms of the spatial frequencies Low resolution High resolution High res/ high noise 11 1 ACF ( x ) L L i( x x' ) i( x' ) dx' NPS( f ) { ACF ( x )} 1 3 3

Image without noise Uncorrelated noise 13 14 Correlated noise Noise and Resolution > SNR Threshold contrast and diameter ~ 1/SNR (Rose model) Higher the SNR > Features w/ smaller C and D can be detected NEQ( f ) SNR actual MTF( f ) NNPS( f ) 15 16 4 4

SNR efficiency Measurement method Best characterized by the detective quantum efficiency (DQE): Efficiency of a detector to utilize the maximum possible SNR provided by the finite number of x-ray photons forming the image Beam quality and magnitude kvp Filtration Exposure Access to linear or linearized data DQE( f ) SNR actual SNR ideal MTF( f ) NNPS( f ) E 0 q 17 18 Al purity Aluminum versus Copper IEC recommendation: >99.9% purity RQA5, 99.0% purity RQA5, 99.99% purity RQA5, 70 kvp 1 mm Al 99.0% purity RQA5, 70 kvp 0.5 mm Cu, 1 mm Al Ranger et al, Med Phys, July 005 19 Murphy et al, AAPM/COMP 011 0 5 5

MTF methodology: Edge Edge test device ESF deduced from image data MTF from ESF via differentiation and Fourier trans. High precision, particularly at low frequencies Simple and quick alignment Established method (endorsed by the IEC) Edge image processing 1. Finding the edge angle Least square fits Differentiation and Hough or Radon transform 1 Edge image processing railabs.org/resources. D projection to obtain ESF 3. ESF differentiation and smoothing to obtain LSF 4. Fourier transformation of LSF to get the presampled MTF 5. Normalization of the MTF at 0 frequency 6. Rebinning the MTF (0.05 mm -1 per IEC) 3 4 6 6

Effect of method (GE XQ/i) Diffs <6% overall <8% single f Opaque edge Slit Trans edge Effect of method (ideal) Diffs <0.3% for slit <5.% for edge Edge Slit True MTF 5 6 Effect of method (w/ glare) Diffs <10% for slit <% for edge Edge Slit True MTF DQE methodology DQE( f ) SNR actual SNR ideal MTF( f ) NNPS( f ) E 0 q MTF > Measured NNPS > Measured E 0 > Measured q (SNR ideal/e 0 ) > Estimated 7 8 7 7

Detector DQE Adding magnification, scatter, grid Grid Tube Patient 9 30 Adding magnification, scatter, grid edqe Ped CXR Adult CXR XL Adult CXR DQE( f ) SNR actual SNR ideal MTF( f ) NNPS( f ) E 0 q edqe( f m ) emtf( f m ) ( 1- SF) ennps( f m ) TF nb E 0 q Samei et al, Med Phys, 009 31 3 8 8

0. 0.18 0.16 0.14 0.1 0.1 0.08 0.06 0.04 0.0 Resolution and contrast transfer From DQE to IQ Image noise: magnitude and texture Attributes of image feature of interest d' ò edqe( f m ).W( f ) fdf Model observers Fisher-Hotelling observer (FH) ' ( d FH ) òò MTF (u,v)w Task (u,v) dudv NPS(u,v) Non-prewhitening observer (NPW) ' [ òò MTF ( d NPW ) (u,v)w Task (u,v) dudv] MTF òò (u,v)w Task (u,v) NPS(u,v)dudv 0 NPW observer with eye filter (NPWE) ' [ òò MTF ( d NPWE ) (u,v)w Task (u,v) E (u,v)dudv] MTF òò (u,v)w Task (u,v) Eye filter 0 0.1 0. 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 NPS(u,v)E 4 (u,v) + MTF (u,v)w Task (u,v)n i dudv Validation of model observers edqe applied to acquisition optimization Richard, Li, Samei, SPIE 011 Boyce et al, Med Phys, 005 36 9 9

10 10 From DQE to IQ and dose: Effective Dose Efficiency (ede) Summary ede( f m ) edqe( f m ) q ES ED æ SSD ö ç è SID ø Samei et al, PMB, 011 medicalphysicsweb.org, July 9, 011 37 MTF can be robustly measured using edge method DQE provides a meaningful measure of detector performance correlated with human performance DQE can be readily extended to system performance (via edqe) DQE can readily be normalized by dose (ede) for acquisition optimization 38