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15
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43049110334
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We used a value of density calculated from the volume of one unit cell.
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We used a value of density calculated from the volume of one unit cell.
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16
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43049099743
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We also compared the profiles of convolved Fig. 2 with profiles of the experimental curve, which is not shown in this Brief Report. The profiles of convolved Fig. 2 showed good agreement only at early time delay, but above 60 ps, it quickly recovered as compared to those of the experimental data.
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We also compared the profiles of convolved Fig. 2 with profiles of the experimental curve, which is not shown in this Brief Report. The profiles of convolved Fig. 2 showed good agreement only at early time delay, but above 60 ps, it quickly recovered as compared to those of the experimental data.
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17
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43049097262
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With a laser fluence of 8 mJ/ cm2, we also checked parameter combinations of ζ and c33 / c13. While the calculation with ζ∼125 nm shows a larger angle change than the experimental result and a quick recovery, the calculation with ζ∼250 nm shows a similar angle shift with the experimental result and Fig. 4.
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With a laser fluence of 8 mJ/ cm2, we also checked parameter combinations of ζ and c33 / c13. While the calculation with ζ∼125 nm shows a larger angle change than the experimental result and a quick recovery, the calculation with ζ∼250 nm shows a similar angle shift with the experimental result and Fig. 4.
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18
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43049109985
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From the sound velocity (7640 m/s) and the x-ray penetration depth (δx, 0.5 μm) at 1.48 keV, we can calculate a time from δx /ν, which approximates the mechanical relaxation time.
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From the sound velocity (7640 m/s) and the x-ray penetration depth (δx, 0.5 μm) at 1.48 keV, we can calculate a time from δx /ν, which approximates the mechanical relaxation time.
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