Literature DB >> 24668520

Two-dimensional imaging in a lightweight portable MRI scanner without gradient coils.

Clarissa Zimmerman Cooley1, Jason P Stockmann, Brandon D Armstrong, Mathieu Sarracanie, Michael H Lev, Matthew S Rosen, Lawrence L Wald.   

Abstract

PURPOSE: As the premiere modality for brain imaging, MRI could find wider applicability if lightweight, portable systems were available for siting in unconventional locations such as intensive care units, physician offices, surgical suites, ambulances, emergency rooms, sports facilities, or rural healthcare sites.
METHODS: We construct and validate a truly portable (<100 kg) and silent proof-of-concept MRI scanner which replaces conventional gradient encoding with a rotating lightweight cryogen-free, low-field magnet. When rotated about the object, the inhomogeneous field pattern is used as a rotating spatial encoding magnetic field (rSEM) to create generalized projections which encode the iteratively reconstructed two-dimensional (2D) image. Multiple receive channels are used to disambiguate the nonbijective encoding field.
RESULTS: The system is validated with experimental images of 2D test phantoms. Similar to other nonlinear field encoding schemes, the spatial resolution is position dependent with blurring in the center, but is shown to be likely sufficient for many medical applications.
CONCLUSION: The presented MRI scanner demonstrates the potential for portability by simultaneously relaxing the magnet homogeneity criteria and eliminating the gradient coil. This new architecture and encoding scheme shows convincing proof of concept images that are expected to be further improved with refinement of the calibration and methodology.
© 2014 Wiley Periodicals, Inc.

Entities:  

Keywords:  Halbach magnet; low-field MRI; nonlinear SEMs; parallel imaging; portable MRI

Mesh:

Year:  2014        PMID: 24668520      PMCID: PMC4257909          DOI: 10.1002/mrm.25147

Source DB:  PubMed          Journal:  Magn Reson Med        ISSN: 0740-3194            Impact factor:   4.668


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