β Scribed by Phillip A. Christiansen; Kenneth S. Pitzer
No coin nor oath required. For personal study only.
Rsccncd 5 Scptcmbcr 198 1 The s~.tttc elcctnc dtpole pohrtzabtittcs for Rb and Cs arc obtancd from iiite-licld SCF and CI calculattons ustng r&ttwstlc cliccttw potentials dovelopcd by Chrtsttanscn et 31 Results agrcr wtth the e~pcrlmcnral v;llucs of hlolol et aI 10 1, tthtn ~5% By contrat, calculauons using Phdhps-Kl(lcmman type potcnttals ior Cs were senously tn error
π SIMILAR VOLUMES
Static electric dipole polarixabilities for helium-like ions H-, He, Li+, Be\*+, B3+, and Ne\*+ are calculated from their respective Hylleraas wavefunctions. However, instead of using the wavefunctions directly, we employ the corresponding densities in a density-based approach proposed recently (by
The static electric dipole polarizabilities and second-order hyperpolarizabilities of several bare boron clusters have been calculated with density functional theory. The average second-order hyperpolarizability Ξ³ av reaches a saturation limit of about 50,000 a.u. already with B 5 for a given type o
The radiation patterns are similar to those of the conventional monopole antenna, although at the fourth band some nulls can be observed and these nulls are deeper for the antenna with ellipticity of 0.5 in the E-plane. In spite of this degradation, the radiation patterns at the fourth band are simi