z-logo
Premium
Influence of proton T 1 on oxymetry using Overhauser enhanced magnetic resonance imaging
Author(s) -
Matsumoto Shingo,
Utsumi Hideo,
Aravalluvan Thirumaran,
Matsumoto Kenichiro,
Matsumoto Atsuko,
Devasahayam Nallathamby,
Sowers Anastasia L.,
Mitchell James B.,
Subramanian Sankaran,
Krishna Murali C.
Publication year - 2005
Publication title -
magnetic resonance in medicine
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.696
H-Index - 225
eISSN - 1522-2594
pISSN - 0740-3194
DOI - 10.1002/mrm.20564
Subject(s) - magnetic resonance imaging , nuclear magnetic resonance , imaging phantom , scanner , physics , pixel , proton , nuclear overhauser effect , computation , zeeman effect , materials science , magnetic field , optics , computer science , algorithm , nuclear magnetic resonance spectroscopy , medicine , nuclear physics , radiology , quantum mechanics
In Overhauser enhanced magnetic resonance imaging (OMRI) for in vivo measurement of oxygen partial pressure ( p O 2 ), a paramagnetic contrast agent is introduced to enhance the proton signal through dynamic nuclear polarization. A uniform proton T 1 is generally assumed for the entire region of interest for the computation of p O 2 using OMRI. It is demonstrated here, by both phantom and in vivo (mice) imaging, that such an assumption may cause erroneous estimate of p O 2 . A direct estimate of pixel‐wise T 1 is hampered by the poor native MR intensities, owing to the very low Zeeman field (15–20 mT) in OMRI. To circumvent this problem, a simple method for the pixel‐wise mapping of proton T 1 using the OMRI scanner is described. A proton T 1 image of a slice through the center of an SCC tumor in a mouse clearly shows a range of T 1 distribution (0.2∼1.6 s). Computation of p O 2 images using pixel‐wise T 1 values promises oximetry with minimal artifacts by OMRI. Magn Reson Med 54:213–217, 2005. Published 2005 Wiley‐Liss, Inc.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom