Rovibronic States in the X2Π State of the CCS− Anion

2003 ◽  
Vol 217 (3) ◽  
pp. 231-240 ◽  
Author(s):  
D. Panten ◽  
G. Chambaud ◽  
P. Rosmus ◽  
E. Riaplov ◽  
J. P. Maier

AbstractThree-dimensional potential energy functions have been generated ab initio for the X2Π electronic ground state of CCS− and used in variational Renner–Teller calculations including electron spin. Rovibronic levels (J=P) for J≤5/2 are given for energies up to 4000cm−1. The pattern of the levels is compared with that of CCO−. In the case of CCS− the quartic force fields, equilibrium geometry, electric dipole moment, the electronic affinity and the Franck–Condon factors for the X2Π(CCS−) → X3Σ− (CCS) photodetachment spectrum are calculated.

2005 ◽  
Vol 04 (01) ◽  
pp. 225-245 ◽  
Author(s):  
IKUO TOKUE ◽  
KATSUYOSHI YAMASAKI ◽  
SATOSHI MINAMINO ◽  
SHINKOH NANBU

To elucidate the ionization dynamics, in particular the vibrational distribution, of H 2 O +(Ã) produced by photoionization and the Penning ionization of H 2 O and D 2 O with He *(2 3S) atoms, Franck–Condon factors (FCFs) were given for the [Formula: see text] ionization, and the transition probabilities were presented for the [Formula: see text] emission. The FCFs were obtained by quantum vibrational calculations using the three-dimensional potential energy surfaces (PESs) of [Formula: see text] and [Formula: see text] electronic states. The global PESs were determined by the multi-reference configuration interaction calculations with the Davidson correction and the interpolant moving least squares method combined with the Shepard interpolation. The obtained FCFs exhibit that the [Formula: see text] state primarily populates the vibrational ground state, as its equilibrium geometry is almost equal to that of [Formula: see text], while the bending mode (ν2) is strongly enhanced for the H 2 O +(Ã) state; the maximums in the population of H 2 O + and D 2 O + are approximately v2 = 11–12 and 15–17, respectively. These results are consistent with the distributions observed by photoelectron spectroscopy. Transition probabilities for the [Formula: see text] system of H 2 O + and D 2 O + show that the bending progressions consist primarily of the [Formula: see text] emission, with combination bands from the (1, v′2 = 4–8, 0) level being next most important.


1993 ◽  
Vol 58 (4) ◽  
pp. 748-753 ◽  
Author(s):  
Narayanan Rajamanickam ◽  
Manuel Fernandez Gomez ◽  
Juan Jesus Lopez Gonzalez

The Franck-Condon factors (vibrational transition probabilities) and r-centroids have been evaluated by a more reliable numerical interogation procedure for the bands of b1Σ+ - X3Σ- system of the PF molecule, using a suitable potential. The dissociation energy, De = 318 kJ mol-1 for the electronic ground state of this molecule has been estimated by fitting the electronegativity function to the experimental potential energy curve.


1985 ◽  
Vol 56 (4) ◽  
pp. 839-851 ◽  
Author(s):  
J.N. Murrell ◽  
W. Craven ◽  
M. Vincent ◽  
Z.H. Zhu

2000 ◽  
Vol 98 (13) ◽  
pp. 875-878 ◽  
Author(s):  
H. Y. Wang ◽  
Z. H. Zhu ◽  
T. Gao ◽  
Y. B. Fu ◽  
X. L. Wang ◽  
...  

1988 ◽  
Vol 43 (3) ◽  
pp. 239-247 ◽  
Author(s):  
C. Sartori ◽  
W. Preetz

The electronic absorption spectrum of the solid tetramethyl-ammonium salt of [OsO2(CN)4]2 - is measured at 10 K. The five distinct band systems exhibit vibrational progressions in the range 660-750 cm - 1, corresponding to the Os = O stretching vibrations sometimes coupled with ν(OsC). From this vibrational fine structure the electronic origin is deduced and verified by characteristic isotopic shifts by 18O and 13C. The two bands at lowest energy are assigned to the d-d-transitions 1A1g [b22g] → 3Eg [b12g e1g] (620 - 460 nm) and 1A1g [b22g] → 1Eg [b12g e1g] (490 - 400 nm). The 3Eg state is split by spin-orbit coupling into 5 components, from the one at lowest energy a luminescence emission (830 - 670 nm) takes place with a progression of 860 cm-1, corresponding to the symmetric Os = O stretching vibration in the electronic ground state. The more intense bands are assigned to charge transfer transitions from oxo π-orbitals into unoccupied niveaus of Os (VI): 1A1g [e4u] → 3A2u [e3u e1g] (390 - 340); → 1A1u [e3u e1g] (340 - 290) and → 1Eu [e3u b11g (290 - 230 nm). The singlet-triplet distances are 3200-3600 cm - 1. From a Franck-Condon analysis an excited state elongation of 10-13 pm for the osmyl groups is calculated.


1985 ◽  
Vol 63 (11) ◽  
pp. 3264-3268 ◽  
Author(s):  
Britta L. Schürmann ◽  
Robert J. Buenker

Abinitio potential curves of the X2A″ ground state and the first excited A2A′ state (2Π in linear geometry) of HNCl are calculated employing multi-reference single- and double-excitation configuration interaction in order to aid in the search for this system experimentally. A vibrational analysis (frequencies and Franck–Condon factors) of the A2A′ – X2A″ transition is undertaken by neglecting coupling between the various modes. Diagonal and off-diagonal force constants together with the fundamental frequencies have been calculated by including mode coupling for both electronic states, and oscillator strengths and radiative lifetimes are also obtained. Comparison with theoretical and experimental results for other isovalent systems is also made in order to establish trends in this group of HAB systems.


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