๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Excited states and photochemistry of saturated molecules. extended basics calculations on the 1B1 (1T2) state of methane

โœ Scribed by Mark S. Gordon


Publisher
Elsevier Science
Year
1977
Tongue
English
Weight
669 KB
Volume
52
Category
Article
ISSN
0009-2614

No coin nor oath required. For personal study only.

โœฆ Synopsis


Ihe surface of the lowest excited smgkt state in meth;lne IS analyzed usmg a basis yet composed of 4-3 IC; augmented by a set of one s and three p Rydbergs. The State (IT2 in Td syrnnrctry. 1 Li, In C 2v! is fmnd to bc dissociatlvc to I B I Cllz and ground state &. Vcrtirally a llydbcrg state, 1B1 rapidly becomes a valence state on dtQortions from tetrahedral syW mctry. Avoided cros\mgs with higher B, SI.I~C~ arc diccusqcd.


๐Ÿ“œ SIMILAR VOLUMES


Excited states and photochemistry of sat
โœ Mark S. Gordon ๐Ÿ“‚ Article ๐Ÿ“… 1976 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 442 KB

Rcccivcd 6 Scptcmber 1976 ST0 4G calculations arc carried out on methane in both tetrahcdrd and l&n-Teller dIstorted Czv and Czv symmctcies. Large incrcascs in Cl1 bond lengths are prcdictcd in al! states, and the r B1 state in Czv symmetry is prcdictcd to dissociate to \* B1 mcthylcne and 'Ai Hz wi

Stretch-Bender Calculations of the Rovib
โœ Geoffrey Duxbury; Alexander Alijah ๐Ÿ“‚ Article ๐Ÿ“… 2002 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 266 KB

The extended stretch-bender Hamiltonian, incorporating spin-orbit coupling and overall rotation, has been used to calculate the spin-vibronic structure of the rovibronic energies in the region where the vibronic states of the excited รƒ 2 A 1 electronic state of NH 2 interact with near-resonant high-

Vibrational excitation of Li2(X 1ฮฃg+) vi
โœ J.M. Wadehra; H.H. Michels ๐Ÿ“‚ Article ๐Ÿ“… 1985 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 306 KB

Cross scct~ons fix vrbrntional c-xltntlon (VE) of the X 1 Z: state of LQ wa formation of the cxnted A '$ or B II-I" eiectromc states are reported. For VE through the A ' ~6 state. the cross secttons are nearly constant for forming X ' ?I; (3 < U" < 9) WI electron colhslonnl cwltatlon. For photon pum