Potential Energy Function and Vibrational States of the Electronic Ground State of N4+

1999 ◽  
Vol 103 (12) ◽  
pp. 1846-1852 ◽  
Author(s):  
Celine Léonard ◽  
Pavel Rosmus ◽  
Stuart Carter ◽  
Nicholas C. Handy
2004 ◽  
Vol 227 (1) ◽  
pp. 1-12 ◽  
Author(s):  
O.N. Ulenikov ◽  
E.S. Bekhtereva ◽  
N.A. Sanzharov ◽  
Per Jensen

2006 ◽  
Vol 55 (5) ◽  
pp. 2175
Author(s):  
Geng Zhen-Duo ◽  
Fan Xiao-Wei ◽  
Zhang Yan-Song

1978 ◽  
Vol 33 (12) ◽  
pp. 1581-1587
Author(s):  
R. N. Kesarwani ◽  
Y. P. Varshni

Abstract A potential energy function is proposed which exhibits a quartic dependence on (r - re), where re is the equilibrium interparticle distance, in the neighbourhood of re, and has a finite binding energy. To study the pattern of the eigenvalues, the WKBJ method is applied to the third order, and the relevant integrals are evaluated analytically. Results are shown graphically for a few sets of parameters. The number of vibrational states that the potential can support is determined for a range of values of the parameters. Some suggestions as to the possible applications of the proposed potential are also made.


1982 ◽  
Vol 37 (9) ◽  
pp. 971-981 ◽  
Author(s):  
G. Van Hooydonk

Abstract The Kratzer-Fues-Varshni-V-potential, applied to ionic dissociation energies, is shown to yield rather accurate potential energy curves in the bonding region for H2, HF, LiH, Li2 and LiF. Vibrational levels, calculated by this ionic approximation to the ground state of widely differing molecules, nearly coincide with RKR-data. At the repulsive side of the curve and up to 2re, the agreement with RKR-curves is even better than for Morse's curve, also for the "covalent" molecules H2 and Li2. Calculated spectroscopical constants αe and ωeχe are far better than those calculated with Morse's function. Even the existence of a maximum in the potential curve at larger r-values seems not in confict with an ionic approximation. From the universal character of the function used, it is concluded that a reasonable approximation for the ground state of all molecules considered is one in terms of ionic structures, even for H2 and especially for Li2. According to the present results, the term “covalent bonding” seems to be definitely superfluous, as the usually made distinction between ionic and covalent bonding is more appearant than real.


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