METHOD FOR OPTIMIZED BIAS AND SIGNAL INFERENCE IN DIFFUSION-WEIGHTED MAGNETIC RESONANCE IMAGE ANALYSIS

作者: Kuczera Stefan , Maier Stephan

DOI:

关键词:

摘要: An approach to estimate noise, Rician signal bias and true in magnitude data obtained with magnetic resonance imaging is proposed. Rather than relying on repeat measurements for estimation of noise expected at given scan parameter settings, the method uses multiple different also referred as weightings, an iterative algorithm associated bias. The fact that behavior response these weightings individual image pixel locations can well be described analytic functions employed infer separate each weighting level measured. Measurements all measured levels contribute ultimate bias-free decay function. Therefore, so processed data, weighted signals computed arbitrary considerably better signal-to-noise ratio originally corresponding weightings. Bias-free desired levels, maps function fit parameters, or a combination such parameters used rapid highly sensitive tissue characterization.

参考文章(5)
Anders Kristoffersen, Optimal estimation of the diffusion coefficient from non-averaged and averaged noisy magnitude data Journal of Magnetic Resonance. ,vol. 187, pp. 293- 305 ,(2007) , 10.1016/J.JMR.2007.05.004
Cheng Guan Koay, Peter J. Basser, Analytically exact correction scheme for signal extraction from noisy magnitude MR signals Journal of Magnetic Resonance. ,vol. 179, pp. 317- 322 ,(2006) , 10.1016/J.JMR.2006.01.016
Ruiliang Bai, Cheng Guan Koay, Elizabeth Hutchinson, Peter J. Basser, A framework for accurate determination of the T2 distribution from multiple echo magnitude MRI images Journal of Magnetic Resonance. ,vol. 244, pp. 53- 63 ,(2014) , 10.1016/J.JMR.2014.04.016
Fredrik Langkilde, Thiele Kobus, Andriy Fedorov, Ruth Dunne, Clare Tempany, Robert V. Mulkern, Stephan E. Maier, Evaluation of fitting models for prostate tissue characterization using extended-range b-factor diffusion-weighted imaging Magnetic Resonance in Medicine. ,vol. 79, pp. 2346- 2358 ,(2018) , 10.1002/MRM.26831