A finite-perturbation method is used for obtaining approximate valence-shell eigenfunctions of molccules interacting with uniform static electric fields within the frame\vork of unrestricted oper;-shell CNDO/II theory. For a series of axially symmetric molecules, components of the polarizability ten
MNDO calculations of molecular electric polarizabilities, hyperpolarizabilities, and nonlinear optical coefficients
β Scribed by Michael J.S. Dewar; Yukio Yamaguchi; Sung Ho Suck
- Publisher
- Elsevier Science
- Year
- 1978
- Tongue
- English
- Weight
- 288 KB
- Volume
- 59
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
β¦ Synopsis
Molecular electric polarizabilities. hyperpo'larizabilities, and nonlinear optical coefficients have been calculated by the MNDO SCF MO method with reasonably satisfactory results.
We recently reported calculations of electric polarizabilities [I] and hyperpolarizabilities [2] for a number of molecules, using the MINDO/3 semiempirical SCF MO method [3] and finite perturbation theory [4]. These quantities can be used to calculate optical properties of crystals and satisfactory results were indeed obtained for the nonlinear optical coefficients of lithium fcrmate monohydrate [.5] .
π SIMILAR VOLUMES
The static dipole polarizability, first and second hyperpolarizability tensors of molecules with nonlinear optical characteristics are calculated via ab initio coupled-perturbed Hartree-Fock theory. A study of the effect of basis set augmentation on the calculated properties for the nitrobenzene mol
The third-order nonlinear optical properties (second molecular hyperpolarizabilities, y), of a series of organoboron compounds containing dimesitylboron moieties have been investigated by third harmonic generation (THG) measurements at 1.907 pm. Symmetric systems with B(mes), groups (mes = 2,4,6-Me,
From a suitable reorganisation of the sum-over-states (SOS) equations of the usual time-independent perturbation theory, recurrent expressions for static polarizability ( a ) and second-( p ) and third-(y) order hyperpolarizabilities are obtained. These expressions are given in a well-adapted way fo