Rotational structure and signature inversion in odd-oddY84

1993 ◽  
Vol 47 (1) ◽  
pp. R1-R4 ◽  
Author(s):  
S. Chattopadhyay ◽  
H. C. Jain ◽  
J. A. Sheikh ◽  
Y. K. Agarwal ◽  
M. L. Jhingan
Keyword(s):  
Rotational Structure ◽  
Signature Inversion

Vibrational and rotational structure in the He i–excited photoelectron spectrum of theAΣ1/2+2state ofHBr+

1994 ◽  
Vol 49 (2) ◽  
pp. 737-744 ◽  
Author(s):  
P. Baltzer ◽  
M. Larsson ◽  
L. Karlsson ◽  
M. Lundqvist ◽  
B. Wannberg
Keyword(s):  
Photoelectron Spectrum ◽  
Rotational Structure

Signature inversion and change in triaxiality inTm159andEr159

1994 ◽  
Vol 49 (1) ◽  
pp. 142-148 ◽  
Author(s):  
Tripti Mathur ◽  
Shankar N. Mukherjee
Keyword(s):  
Signature Inversion

Search for Signature Inversion of Yrast Band in Odd-Odd 162Lu Nucleus

1996 ◽  
Author(s):  
Zhang Yuhu ◽  
Zhou Xiaohong ◽  
Zhao Qingzhong ◽  
Sun Xiangfu ◽  
Lei Xiangguo ◽  
...  
Keyword(s):  
Yrast Band ◽  
Signature Inversion

Levels, transitions and rotational structure in 227Ac

1969 ◽  
Vol 124 (2) ◽  
pp. 412-428 ◽  
Author(s):  
R.C. Lange ◽  
G.R. Hagee
Keyword(s):  
Rotational Structure

THE ABSORPTION SPECTRUM OF CF2

1967 ◽  
Vol 45 (7) ◽  
pp. 2355-2374 ◽  
Author(s):  
C. Weldon Mathews
Keyword(s):  
Absorption Spectrum ◽  
Electronic State ◽  
Ground State ◽  
Band System ◽  
Electronic States ◽  
Vibrational Structure ◽  
Rotational Structure ◽  
Transition Moment ◽  
High Dispersion ◽  
Parallel Type

The absorption spectrum of CF2 in the 2 500 Å region has been photographed at high dispersion, and the rotational structure of a number of bands has been analyzed. The analysis of the well-resolved subbands establishes that these are perpendicular- rather than parallel-type bands, as previously assigned. Further analysis shows that the upper and lower electronic states are of 1B1 and 1A1symmetries respectively, corresponding to a transition moment that is perpendicular to the plane of the molecule. In the upper electronic state, r0(CF) = 1.32 Å and [Formula: see text], while in the ground state, r0(CF) = 1.300 Å and [Formula: see text]. An investigation of the vibrational structure of the band system has shown that the vibrational numbering in ν2′ must be increased by one unit from earlier assignments, thus placing the 000–000 band near 2 687 Å (37 220 cm−1). A search between 1 300 and 8 500 Å showed two new band systems near 1 350 and 1 500 Å which have been assigned tentatively to the CF2 molecule.

Re-analysis of the (100), (001), and (020) rotational structure of SO2 on the basis of high resolution FTIR spectra

2013 ◽  
Vol 130 ◽  
pp. 220-232 ◽  
Author(s):  
O.N. Ulenikov ◽  
G.A. Onopenko ◽  
O.V. Gromova ◽  
E.S. Bekhtereva ◽  
V.-M. Horneman
Keyword(s):  
High Resolution ◽  
Ftir Spectra ◽  
Rotational Structure

Theoretical calculations of electronic Raman effects of the NO and O2 molecules

1970 ◽  
Vol 48 (14) ◽  
pp. 1664-1674 ◽  
Author(s):  
D. W. Lepard
Keyword(s):  
Raman Spectrum ◽  
Raman Spectra ◽  
Theoretical Calculations ◽  
Diatomic Molecules ◽  
Wave Functions ◽  
Rotational Structure ◽  
Intermediate Case ◽  
First Time

This paper presents a method for calculating the relative intensities and Raman shifts of the rotational structure in electronic Raman spectra of diatomic molecules. The method is exact in the sense that the wave functions used for the calculations may belong to any intermediate case of Hund's coupling schemes. Using this method, theoretical calculations of the pure rotational and electronic Raman spectrum of NO, and the pure rotational Raman spectrum of O2, are presented. Although a calculated stick spectrum for NO was previously shown by Fast et al., the details of this calculation are given here for the first time.

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