R−K−R−V potential energy curve, Franck— Condon factors andr-centroids forE 1 Σ +-X 1 Σ + system of SiS molecule

1975 ◽  
Vol 39 (3) ◽  
pp. 145-148
Author(s):  
P. H. Katti ◽  
V. M. Korwar



1992 ◽  
Vol 70 (9) ◽  
pp. 764-771 ◽  
Author(s):  
G. P. Mishra ◽  
V. B. Singh ◽  
S. B. Rai

The fine structure of the D–X system of the CuI molecule has been reinvestigated following a doubtful and incomplete analysis of this system by Nair and Upadhya. The rotational structure was photographed in emission in the second order of a 10.6 m grating spectrograph with 0.33 Å/mm dispersion. Though the transition of the system was found to be the same as suggested by Nair and Upadhya, the molecular constants are considerably modified. The various molecular constants (cm−1) determined for the D1π state by using a weighted least-squares-fit computer program are as follows: Bc, 0.067 040(4); αc, 0.000 420(4); Dc, 0.250 × 10−7(3); q, −0.000 272(1); rc, 2.445 02(6) Å (1 Å = 10−10 m). The potential energy curve for the D1π state and Franck–Condon factors and r-centroids for the D–X system have also been reported.



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.



2012 ◽  
Vol 116 (7) ◽  
pp. 1717-1729 ◽  
Author(s):  
Laimutis Bytautas ◽  
Nikita Matsunaga ◽  
Gustavo E. Scuseria ◽  
Klaus Ruedenberg


1977 ◽  
Vol 66 (3) ◽  
pp. 1135-1140 ◽  
Author(s):  
Luis R. Kahn ◽  
Thom H. Dunning ◽  
Nicholas W. Winter ◽  
William A. Goddard


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.



1999 ◽  
Vol 461-462 ◽  
pp. 351-357 ◽  
Author(s):  
Yoshi-ichi Suzuki ◽  
Takeshi Noro ◽  
Fukashi Sasaki ◽  
Hiroshi Tatewaki




2015 ◽  
Vol 17 (9) ◽  
pp. 6374-6382 ◽  
Author(s):  
Anna Amat ◽  
Costanza Miliani ◽  
Aldo Romani ◽  
Simona Fantacci

Potential energy curve for the ESIPT. Top inset: vibrationally resolved emission spectra computed for both tautomers. Bottom insets: main vibrational modes.



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