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Dipole,quadrupole, octupole,and dipole–dipole–quandrupole polarizabilities and second hyperpolarizabilities at real and imaginary frequencies for helium in the 23S state: Dispersion-energy coefficients for interactions between He(23S) and H(12S), He(11S), He(23S), or H2(X1∑g+)
Authors:David M Bishop  Janusz Pipin
Abstract:We have determined the dynamic dipole (α1), quadrupole (α2), octupole (α3), and dipole–dipole–quadrupole (B) polarizabilities and the second hyperpolarizability tensor (γ) for the helium atom in its lowest triplet state (23S). We have done so for both real and imaginary frequencies: in the former case, for a range of frequencies (ω) between zero and the first electronic-transition frequency, and in the latter case for a 32-point Gauss–Legendre grid running from zero to ?ω = 20 Eh. We have also determined the dispersion-energy coefficients C6, C8, and C10 for the systems H(12S)? He(23S), He(11S)? He(23S), and He(23S)? He(23S) and the Curn:x-wiley:00207608:media:QUA560470204:tex2gif-stack-1, Curn:x-wiley:00207608:media:QUA560470204:tex2gif-stack-2, Curn:x-wiley:00207608:media:QUA560470204:tex2gif-stack-3, Curn:x-wiley:00207608:media:QUA560470204:tex2gif-stack-4, and Curn:x-wiley:00207608:media:QUA560470204:tex2gif-stack-5 coefficients for the interaction He(23S)? H2(X1urn:x-wiley:00207608:media:QUA560470204:tex2gif-stack-6). Our values of the higher-order multipolar polarizabilities and of γ for the 23S state of helium are, we believe, the first to be published. © 1993 John Wiley & Sons, Inc.
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