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Controlling diffusion of 3 He by buffer gases: A structural contrast agent in lung MRI
Author(s) -
Acosta Rodolfo H.,
Blümler Peter,
AgullesPedrós Luis,
Morbach Andreas E.,
Schmiedeskamp Jörg,
Herweling Annette,
Wolf Ursula,
Scholz Alexander,
Schreiber Wolfgang G.,
Heil Werner,
Thelen Manfred,
Spiess HansWolfgang
Publication year - 2006
Publication title -
journal of magnetic resonance imaging
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.563
H-Index - 160
eISSN - 1522-2586
pISSN - 1053-1807
DOI - 10.1002/jmri.20777
Subject(s) - diffusion , effective diffusion coefficient , buffer gas , molecular diffusion , inert gas , contrast (vision) , signal (programming language) , resolution (logic) , materials science , nuclear magnetic resonance , gaseous diffusion , diffusion mri , chemistry , analytical chemistry (journal) , laser , magnetic resonance imaging , optics , physics , thermodynamics , chromatography , radiology , computer science , operations management , artificial intelligence , metric (unit) , composite material , programming language , medicine , electrode , economics
Purpose To study the influence of admixing inert buffer gases to laser‐polarized 3 He in terms of resulting diffusion coefficients and the consequences for image contrast and resolution. Materials and Methods The diffusion coefficient of 3 He was altered by admixing buffer gases of various molecular weights ( 4 He, N 2 , and SF 6 ). The influence of the pulse sequence and the diffusion coefficient on the appearance of MRI of (laser‐polarized) gases was analyzed by comparison of basic theoretical concepts with demonstrative experiments. Results Excellent agreement between theoretical description and observed signal in simple gradient echoes was observed. A maximum signal gain can be predicted and was experimentally validated. Images acquired under such conditions revealed improved resolution. The nature and concentration of the admixed gas defines a structural threshold for the observed apparent diffusion coefficient (ADC) as demonstrated with diffusion‐weighted MRI on a pig's lung flooded with suitable gas mixtures. Conclusion A novel procedure is proposed to control the diffusion coefficient of gases in MRI by admixture of inert buffer gases. Their molecular mass and concentration enter as additional parameters into the equations that describe structural contrast. This allows for setting a structural threshold up to which structures contribute to the image. For MRI of the lung this enables images of very small structural elements (alveoli) only, or in the other extreme, all airways can be displayed with minimal signal loss due to diffusion. J. Magn. Reson. Imaging 2006. © 2006 Wiley‐Liss, Inc.