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Spatial backward planar projection in absorbing media possessing an arbitrary dispersion relation.

Acoustical science and technology; DOI:10.1250/ast.31.379

Planar projection methods have been shown to rapidly relate fields between two planes. Such an approach is particularly useful for characterizing transducers, since only a single plane needs to be measured in order to characterize an entire field. The present work considers the same approach in the presence of an arbitrary dispersion relation. Unlike traditional methods that use Fourier solutions of the time-domain wave equation, the approach starts from a frequency-domain Helmholtz equation for waves in a dispersive medium. It is shown that a transfer function similar to that derived from time domain equations can be utilized. Both the forward- and backward-projection behaviors are examined and it is demonstrated that the approach is invariant to propagation direction.
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Copyright © 2010 Acoustical Society of Japan

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Clinic Ultrasound Laboratory (クレメント超音波研究室)
Cleveland Clinic (クリーブランド・クリニック),
Lerner Research Institute
Case Western Reserve University
© 2014

Research interest

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Highlighted Publications

For a comprehensive listing see PUBLICATIONS

Clement GT, Nomura H, Adachi H,  Kamakura T, Feasibility of non-contact ultrasound for medical imaging, Physics in Medicine and Biology 2014; 58: 6263-6278 

Tang SC, Jolesz FA, Clement GT.  A Wireless Batteryless  Implantable Ultrasonic Pulser-Receiver.  IEEE Trans Ultrason Ferroelectr Freq Control 2011;58:1211-21.

Paltiel HJ, Padua HM, Gargollo PC, Cannon GM Jr, Alomari AI, Yu R, Clement GT. Volumetric ultrasound imaging of tissue perfusion: preliminary results in a rabbit model... Phys Med Biol 2011;56:2183-97.

McDannold N, Clement GT, Black P, Jolesz F, Hynynen K.  Focused ultrasound surgery of brain tumors: Initial findings in three patients. Neurosurgery 2010;66:323-32; discussion 332.

Clement GT, Hynynen K. A non-invasive method for focusing ultrasound through the human skull. Phys Med Biol 2002;47(8):1219-36.

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