programa computacional stata Search Results


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Remcom Inc xfdtd software
Quantitative B1+ maps (nT/ampere) of the center transverse slice of the head derived from <t>FDTD-simulated</t> fields. Each map exhibits severe inhomogeneity. Sp(r) is the B1+ field that arises when channel p is driven with a 1-ampere peak-to-peak 300-MHz sinusoid.
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ANSYS inc fdtd module in the ansys lumerical software
Quantitative B1+ maps (nT/ampere) of the center transverse slice of the head derived from <t>FDTD-simulated</t> fields. Each map exhibits severe inhomogeneity. Sp(r) is the B1+ field that arises when channel p is driven with a 1-ampere peak-to-peak 300-MHz sinusoid.
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CAMO Software unscrambler® from camo software
Quantitative B1+ maps (nT/ampere) of the center transverse slice of the head derived from <t>FDTD-simulated</t> fields. Each map exhibits severe inhomogeneity. Sp(r) is the B1+ field that arises when channel p is driven with a 1-ampere peak-to-peak 300-MHz sinusoid.
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TURBOMOLE GmbH turbomole v6.0
Quantitative B1+ maps (nT/ampere) of the center transverse slice of the head derived from <t>FDTD-simulated</t> fields. Each map exhibits severe inhomogeneity. Sp(r) is the B1+ field that arises when channel p is driven with a 1-ampere peak-to-peak 300-MHz sinusoid.
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Image Search Results


Quantitative B1+ maps (nT/ampere) of the center transverse slice of the head derived from FDTD-simulated fields. Each map exhibits severe inhomogeneity. Sp(r) is the B1+ field that arises when channel p is driven with a 1-ampere peak-to-peak 300-MHz sinusoid.

Journal:

Article Title: Specific Absorption Rate Studies of the Parallel Transmission of Inner-Volume Excitations at 7 Tesla

doi: 10.1002/jmri.21548

Figure Lengend Snippet: Quantitative B1+ maps (nT/ampere) of the center transverse slice of the head derived from FDTD-simulated fields. Each map exhibits severe inhomogeneity. Sp(r) is the B1+ field that arises when channel p is driven with a 1-ampere peak-to-peak 300-MHz sinusoid.

Article Snippet: We obtain these via 300-MHz FDTD simulations (XFDTD software, REMCOM Inc., State College, PA, USA), and then evaluate the SAR of any given excitation by superimposing modulated versions of these electric fields ( 5 , 18 , 30 , 31 ), avoiding the computationally-intractable scenario of FDTD-simulating each of the 200+ pTX excitations evaluated in this paper.

Techniques: Derivative Assay