The D–X system of the CuI molecule

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.



1976 ◽  
Vol 54 (18) ◽  
pp. 1898-1904 ◽  
Author(s):  
Walter J. Balfour ◽  
Hugh M. Cartwright

The B′2Σ+ → X2Σ+ systems in MgH and MgD have been studied in emission at high resolution. Vibrational and rotational analyses, which have been performed for 37 bands of MgH and 16 bands of MgD, provide data on the following vibrational levels of the B′ state: MgH, ν = 0–9; MgD, ν = 0–2, 4–6. The following molecular constants (in cm−1) have been determined for the B′ state: MgH, Tc = 22 410, ωc = 828.4, ωcxc = 11.8, Bc = 2.585, Dc = 1.2 × 10−4; MgD, Tc = 22 415, ωc = 598.1, ωcxc = 6.4, Bc = 1.346, Dc = 2.6 × 10−5. The dissociation energy, Dc, in the B′ state is estimated to be 10 900 cm−1 (MgH), 11 200 cm−1 (MgD). The RKR potential energy curve for the B′ state has been calculated. A correlation of the rotational perturbations in the B′ → X system with the positions of rotational energy levels in the A2Π and B′2Σ+ states has been made. Observations for the low-lying states of MgH are compared with similar available data for related hydrides.





1983 ◽  
Vol 61 (4) ◽  
pp. 641-655 ◽  
Author(s):  
R. Colin ◽  
C. Dreze ◽  
M. Steinhauer

A new C2Σ+–X2Σ+ transition of BeH and BeD is observed in a beryllium are in hydrogen or deuterium gas mixed with argon. The rotational analysis of the most intense of these strongly red degraded bands, which involve ν′ = 0–2 for BeH and ν′ = 0 for BeD, allows one to derive molecular constants for the new C2Σ+ state. The latter has a large internuclear equilibrium distance (re = 2.301 Å) and a shallow potential energy minimum [Formula: see text]. The principal molecular constants determined are:C2Σ+Tc = 30 953.94 cm−1[Formula: see text]Rotational perturbations between the C2Σ+ and A2Π states are observed in the C–X bands of BeH and BeD and in two new A–X bands of BeH (4–4 and 5–5) which have also been observed and analyzed. These perturbations are treated by a matrix approach and yield a value for the interaction matrix element [Formula: see text].The C–X bands analyzed involve the higher vibrational levels of the X2Σ+ state and allow, therefore, a substantial improvement of the ground state molecular constants to be made and a good Rydberg–Klein–Rees (RKR) potential energy curve to be calculated. The limiting curve of the predissociation confirms the previous value of the dissociation energy [Formula: see text] and indicates that a small maximum, less than 200 cm−1, could exist at [Formula: see text] in the ground state potential energy curve.Franck–Condon factors for the C2Σ+–X2Σ+ bands of BeH and BeD are also calculated.



1979 ◽  
Vol 57 (3) ◽  
pp. 496-504 ◽  
Author(s):  
B. R. Yadav ◽  
S. B. Rai ◽  
D. K. Rai

The electronic spectrum of the GaO molecule has been re-investigated in the region 3600–4200 Å The use of high resolution and dispersion permitted clear resolution of the rotational structure and the formation of head of heads in Δν = + 1 and + 2 sequences is clearly visible. The rotational analyses of the (0,0) and the (1,0) bands have been performed and more reliable molecular constants have been obtained. Intensity anomalies in the bands have been explained on the basis of the true potential energy curves and the associated Franck–Condon factors.



1998 ◽  
Vol 189 (2) ◽  
pp. 244-248 ◽  
Author(s):  
V. Bednarska ◽  
I. Jackowska ◽  
W. Jastrzębski ◽  
P. Kowalczyk


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