A theory is presented for the second term of the series representing the asymptotic atom-surface interaction: V(z) ∼ - C 3(z - z0)-3 - C5(z - z0)-5... The expression for C5 is analogous to that for C3, with the quadrupole polarizability y replacing the dipole polarizability α. Numerical results are obtained for H, Na, Cs and noble gas atoms interactin
THE DISPERSION FORCE OF PHYSICAL ADSORPTION .2. NONLOCAL THEORY
TOIGO, FLAVIO;
1984
Abstract
A theory is presented for the second term of the series representing the asymptotic atom-surface interaction: V(z) ∼ - C 3(z - z0)-3 - C5(z - z0)-5... The expression for C5 is analogous to that for C3, with the quadrupole polarizability y replacing the dipole polarizability α. Numerical results are obtained for H, Na, Cs and noble gas atoms interactin
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