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The deviation from 1 in the correlation of independent measurements for the same real image pattern is a measure of the overall scale of image relief relative to the random noise contribution in the frames. Thus, a flatter image, relative to the noise, will have a smaller γ value for independently recorded frames; see, for example, the slight difference in baseline values in Fig. 2C
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The deviation from 1 in the correlation of independent measurements for the same real image pattern is a measure of the overall scale of image relief relative to the random noise contribution in the frames. Thus, a flatter image, relative to the noise, will have a smaller γ value for independently recorded frames; see, for example, the slight difference in baseline values in Fig. 2C.
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56749144730
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The width rises because of the induced structural inhomogeneity, as expected, and near t = 0 an initial decrease is noted, which indicates that the overall temporal response is much faster than that of the amplitude or separation rise.
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The width rises because of the induced structural inhomogeneity, as expected, and near t = 0 an initial decrease is noted, which indicates that the overall temporal response is much faster than that of the amplitude or separation rise.
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We have calculated the maximum strain-induced tilt angle of the surface normal and found it to be φ ≅ √6ΔL/L. For ΔL/L, 0.043, φ, 2.9°, and the corresponding bulge reaches 1 to 10 nm when the local (lateral) deformation scale is 0.08 to 0.8 μm. For the nanosecond heating at a fluence of 40 mJ/cm2 (Fig. 2F, the Bragg spot separation change is ∼1, giving φ, 14°. The calculated angles correspond well to the angles of microscope specimen tilt needed to produce diffraction and contrast changes similar to those caused by heating. The lateral expansion of ΔL/L, 0.043% after fs heating gives, at equilibrium, a temperature change of 30 K, using α, 14.2 × 10?6 K?1. A higher ΔT derived from the intensity changes (Debye-Waller factor) may have some contribution from zone-axis tilt. Because the zone axis was along the [100] direction before the arrival of th
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?1. A higher ΔT derived from the intensity changes (Debye-Waller factor) may have some contribution from zone-axis tilt. Because the zone axis was along the [100] direction before the arrival of the heat impulse, the influence of tilting would make the derived ΔT a maximum value.
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We thank F. Carbone for his handling of the graphite film and for helpful discussion. This work was supported by the National Science Foundation and Air Force Office of Scientific Research in the Gordon and Betty Moore Center for Physical Biology at Caltech. Research on biological UEM imaging was supported by the National Institutes of Health. Caltech has filed a provisional patent application for the microscope described here
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We thank F. Carbone for his handling of the graphite film and for helpful discussion. This work was supported by the National Science Foundation and Air Force Office of Scientific Research in the Gordon and Betty Moore Center for Physical Biology at Caltech. Research on biological UEM imaging was supported by the National Institutes of Health. Caltech has filed a provisional patent application for the microscope described here.
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