Generalizing the MTF and DQE to include x-ray scatter and focal spot unsharpness: Application to a new microangiographic system

被引:74
作者
Kyprianou, LS [1 ]
Rudin, S
Bednarek, DR
Hoffmann, KR
机构
[1] SUNY Buffalo, Toshiba Stroke Res Ctr, Buffalo, NY 14214 USA
[2] Dept Phys, Buffalo, NY 14214 USA
[3] Dept Radiol, Buffalo, NY 14214 USA
[4] Dept Neurol, Buffalo, NY 14214 USA
关键词
D O I
10.1118/1.1844151
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 [临床医学]; 100207 [影像医学与核医学]; 1009 [特种医学];
摘要
Detector characterization with modulation transfer function (MTF) and detective quantum efficiency (DQE) inadequately predicts image quality when the imaging system includes focal spot unsharpness and patient scatter. The concepts of MTF, noise power spectrum, noise equivalent quanta and DQE were referenced to the object plane and generalized to include the effect of geometric unsharpness due to the finite size of the focal spot and the effect of the spatial distribution and magnitude of x-ray scatter due to the patient. The generalized quantities provide performance characteristics that consider the complete imaging system, but reduce to a description of the detector properties without magnification or scatter. We have evaluated a new neurovascular angiography imaging system based on a region of interest (ROI) microangiographic detector using these generalized quantities. A uniform head-equivalent phantom was used as a filter and x-ray scatter source. This allowed the study of all properties of the detector under clinically relevant x-ray spectra and x-ray scatter conditions. Realistic focal spots (0.8 mm nominal), beam energies (60-100 kVp), and detector exposures (0.8-2.3 mR) were used, and the effects of different scatter fractions (0-0.62) resulting from changing the beam size (0-100 cm(2)) were investigated. The generalized MTF and DQE were found to have very little dependence on the tube voltage and the detector entrance exposure. Magnification, with the focal spot used, results in a large decrease of the generalized DQE at higher frequencies (about 100-fold at 10 cycles/mm), but a significantly smaller decrease at lower frequencies. Scatter on the other hand, causes a constant drop in the generalized DQE (factor of 3 for scatter fraction 0.3) for all frequencies. Our results show that there are tradeoffs in the choice of the different system parameters; therefore this methodology of studying the imaging system as a whole could provide guidance in system design. (C) 2005 American Association of Physicists in Medicine.
引用
收藏
页码:613 / 626
页数:14
相关论文
共 48 条
[1]
[Anonymous], INTRO PHYS DIAGNOSTI
[2]
Evaluation of the imaging properties of two generations of a CCD-based system for digital chest radiography [J].
Båth, M ;
Sund, P ;
Månsson, LG .
MEDICAL PHYSICS, 2002, 29 (10) :2286-2297
[3]
Bednarek D. R., 1985, Proceedings of the SPIE - The International Society for Optical Engineering, V555, P13, DOI 10.1117/12.949462
[4]
ARTIFACTS PRODUCED BY MOVING GRIDS [J].
BEDNAREK, DR ;
RUDIN, S ;
WONG, R .
RADIOLOGY, 1983, 147 (01) :255-258
[5]
Boone J. M., 2000, HDB MED IMAGING, V1, P3
[6]
CHARACTERIZATION OF THE POINT SPREAD FUNCTION AND MODULATION TRANSFER-FUNCTION OF SCATTERED RADIATION USING A DIGITAL IMAGING-SYSTEM [J].
BOONE, JM ;
ARNOLD, BA ;
SEIBERT, JA .
MEDICAL PHYSICS, 1986, 13 (02) :254-256
[8]
Accurate method for computer-generating tungsten anode x-ray spectra from 30 to 140 kV [J].
Boone, JM ;
Seibert, JA .
MEDICAL PHYSICS, 1997, 24 (11) :1661-1670
[9]
Brezovich I A, 1977, Med Phys, V4, P451, DOI 10.1118/1.594315
[10]
BUHR E, 2003, P SOC PHOTO-OPT INS, V5030, P5030