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@ARTICLE{Demberg:119835,
author = {K. Demberg$^*$ and F. Laun$^*$ and J. Windschuh$^*$ and R.
Umathum$^*$ and P. Bachert$^*$ and T. A. Kuder$^*$},
title = {{N}uclear magnetic resonance diffusion pore imaging:
{E}xperimental phase detection by double diffusion
encoding.},
journal = {Physical review / E},
volume = {95},
number = {2},
issn = {2470-0045},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {DKFZ-2017-00430},
pages = {022404},
year = {2017},
abstract = {Diffusion pore imaging is an extension of
diffusion-weighted nuclear magnetic resonance imaging
enabling the direct measurement of the shape of arbitrarily
formed, closed pores by probing diffusion restrictions using
the motion of spin-bearing particles. Examples of such pores
comprise cells in biological tissue or oil containing
cavities in porous rocks. All pores contained in the
measurement volume contribute to one reconstructed image,
which reduces the problem of vanishing signal at increasing
resolution present in conventional magnetic resonance
imaging. It has been previously experimentally demonstrated
that pore imaging using a combination of a long and a narrow
magnetic field gradient pulse is feasible. In this work, an
experimental verification is presented showing that pores
can be imaged using short gradient pulses only. Experiments
were carried out using hyperpolarized xenon gas in
well-defined pores. The phase required for pore image
reconstruction was retrieved from double diffusion encoded
(DDE) measurements, while the magnitude could either be
obtained from DDE signals or classical diffusion
measurements with single encoding. The occurring image
artifacts caused by restrictions of the gradient system,
insufficient diffusion time, and by the phase reconstruction
approach were investigated. Employing short gradient pulses
only is advantageous compared to the initial long-narrow
approach due to a more flexible sequence design when
omitting the long gradient and due to faster convergence to
the diffusion long-time limit, which may enable application
to larger pores.},
cin = {E020},
ddc = {530},
cid = {I:(DE-He78)E020-20160331},
pnm = {315 - Imaging and radiooncology (POF3-315)},
pid = {G:(DE-HGF)POF3-315},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:28298006},
doi = {10.1103/PhysRevE.95.022404},
url = {https://inrepo02.dkfz.de/record/119835},
}