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- W2023584596 startingPage "651" @default.
- W2023584596 abstract "The linear response of the optical constants of Cu to a general strain is presented for the range $1.5ensuremath{le}ensuremath{hbar}ensuremath{omega}ensuremath{le}5.5$ eV. The transitions ${X}_{5}ensuremath{rightarrow}{{X}_{4}}^{ensuremath{'}}$ at 4.0 eV and ${E}_{F}ensuremath{rightarrow}{L}_{1}$ at 4.15 eV are identified. The deformation potentials $frac{ensuremath{partial}({E}_{F}ensuremath{-}{{L}_{3}}^{mathrm{upper}})}{ensuremath{partial}e}=ensuremath{-}(1.1ifmmodepmelsetextpmfi{}0.1)$ eV and $frac{ensuremath{partial}({L}_{1}ensuremath{-}{E}_{F})}{ensuremath{partial}e}=ensuremath{-}(9.6ifmmodepmelsetextpmfi{}1.5)$ eV with $e=frac{ensuremath{Delta}V}{V}$, and $frac{ensuremath{partial}{L}_{1}}{ensuremath{partial}{e}_{mathrm{yz}}}=ensuremath{-}(72ifmmodepmelsetextpmfi{}12)$ eV with ${e}_{mathrm{xy}}={e}_{mathrm{yz}}={e}_{mathrm{zx}}$, ${e}_{mathrm{xx}}={e}_{mathrm{yy}}={e}_{mathrm{zz}}=0$ for kensuremath{parallel}[111] are evaluated from the measurements. They are used to derive the volume coefficients of the Fermi energy, $frac{ensuremath{partial}(mathrm{ln}{E}_{F})}{ensuremath{partial}e}=ensuremath{-}1.1ifmmodepmelsetextpmfi{}0.3$, and of the position of the $d$ bands, $frac{ensuremath{partial}(mathrm{ln}{E}_{d})}{ensuremath{partial}e}=ensuremath{-}1.2ifmmodepmelsetextpmfi{}0.5$, with respect to ${ensuremath{Gamma}}_{1}$. The measurements are consistent with the assumption that direct interband transitions dominate the absorption above 2 eV." @default.
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- W2023584596 date "1968-08-15" @default.
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- W2023584596 title "Effect of Uniaxial and Hydrostatic Strain on the Optical Constants and the Electronic Structure of Copper" @default.
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