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0 should be excluded to avoid fictitious short-wavelength noise currents and thus to make the inversion scheme stable (16). We set (victory hand) = 0.8 μm. but because (victory hand) is much smaller than the spatial resolution of our MO technique, the calculated J(r) only very weakly depends on (victory hand).
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note
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The work at University of Wisconsin was supported by the NSF Materials Research Group Program (DMR 9214707) and the Electric Power Research Institute (RP 8009-5). The work at Oak Ridge National Laboratory is managed by Lockheed Martin Energy Research for the U.S. Department of Energy (DOE) under contract DE-AC05-96OR22464. The work was partly conducted at the National Synchrotron Light Source, which is supported by DOE under contract DE-AC02-76CH00016.
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