Screen optics effects on detective quantum efficiency in digital radiography: zero-frequency effects.

Indirect flat panel imagers have been developed for digital radiography, fluoroscopy and mammography, and are now in clinical use. Screens made from columnar structured cesium iodide (CsI) scintillators doped with thallium have been used extensively in these detectors. The purpose of this article is to investigate the effect of screen optics, e.g., light escape efficiency versus depth, on gain fluctuation noise, expressed as the Swank factor. Our goal is to obtain results useful in optimizing screens for digital radiography systems. Experimental measurements from structured CsI samples were used to derive their screen optics properties, and the same methods can also be applied to powder screens. CsI screens, all of the same thickness but with different optical designs and manufacturing techniques, were obtained from Hamamatsu Photonics Corporation. The pulse height spectra (PHS) of the screens were measured at different x-ray energies. A theoretical model was developed for the light escape efficiency and a method for deriving light escape efficiency versus depth from experimental PHS measurements was implemented and applied to the CsI screens. The results showed that the light escape efficiency varies essentially linearly as a function of depth in the CsI samples, and that the magnitude of variation is relatively small, leading to a high Swank factor.

[1]  Aldo Badano,et al.  Depth-dependent phosphor blur in indirect x-ray imaging sensors , 2002, SPIE Medical Imaging.

[2]  J A Rowlands,et al.  Digital radiology using active matrix readout of amorphous selenium: theoretical analysis of detective quantum efficiency. , 1997, Medical physics.

[3]  Goran Ristic,et al.  X-ray imaging performance of structured cesium iodide scintillators. , 2004, Medical physics.

[4]  J Yorkston,et al.  Signal, noise power spectrum, and detective quantum efficiency of indirect-detection flat-panel imagers for diagnostic radiology. , 1998, Medical physics.

[6]  Donald Michael Korn,et al.  Storage Phosphor System For Computed Radiography: Screen Optics , 1986, Other Conferences.

[7]  R. K. Swank,et al.  Calculation of modulation transfer functions of x-ray fluorescent screens. , 1973, Applied optics.

[8]  J Yorkston,et al.  Empirical investigation of the signal performance of a high-resolution, indirect detection, active matrix flat-panel imager (AMFPI) for fluoroscopic and radiographic operation. , 1997, Medical physics.

[9]  David P. Trauernicht,et al.  The Measurement Of Conversion Noise In X-Ray Intensifying Screens , 1988, Medical Imaging.

[10]  A. Schuster Radiation through a foggy atmosphere , 1903 .

[11]  J A Rowlands,et al.  Optical factors affecting the detective quantum efficiency of radiographic screens. , 1986, Medical physics.

[12]  David P. Trauernicht,et al.  Screen design for flat-panel imagers in diagnostic radiology , 1998, Medical Imaging.

[13]  Li Yang,et al.  Revised Kubelka-Munk theory. III. A general theory of light propagation in scattering and absorptive media. , 2005, Journal of the Optical Society of America. A, Optics, image science, and vision.

[14]  R. K. Swank Absorption and noise in x‐ray phosphors , 1973 .

[15]  J A Rowlands,et al.  Effects of characteristic x rays on the noise power spectra and detective quantum efficiency of photoconductive x-ray detectors. , 2001, Medical physics.

[16]  C E Dick,et al.  Image information transfer properties of x-ray fluorescent screens. , 1981, Medical physics.

[17]  John A. Rowlands,et al.  Effect of depth-dependent modulation transfer function and K-fluorescence reabsorption on the detective quantum efficiency of indirect-conversion flat-panel x-ray imaging systems using CsI , 2001, SPIE Medical Imaging.