Franck—Condon factors,r-centroids and electronic transition moment variation with internuclear distance for AlO (A 2 Σ−X 2Σ) band system using RKR potentials

1981 ◽  
Vol 50 (1) ◽  
pp. 103-120 ◽  
Author(s):  
N. R. Tawde ◽  
V. G. Tulasigeri
Keyword(s):  
Internuclear Distance ◽  
Electronic Transition ◽  
Band System ◽  
Transition Moment ◽  
Electronic Transition Moment ◽  
Condon Factors ◽  
Franck Condon

AN EXPERIMENTAL STUDY OF THE BAND INTENSITIES IN THE CN RED SYSTEM

1958 ◽  
Vol 36 (1) ◽  
pp. 127-133 ◽  
Author(s):  
R. N. Dixon ◽  
R. W. Nicholls
Keyword(s):  
Experimental Study ◽  
Carbon Tetrachloride ◽  
Electronic Transition ◽  
Transition Moment ◽  
Active Nitrogen ◽  
Electronic Transition Moment ◽  
System A ◽  
Condon Factors ◽  
Franck Condon

Experimental band intensities in the CN red system, A (2Πi) →X(2Σ+), have been measured using an active nitrogen – carbon tetrachloride source. Using calculated Franck–Condon factors qν′ν″ the electronic transition moment Re(r) is found to vary little over the range 1.04 < r < 1.27 Å.

Variation of the Electronic Transition Moment and the Effective Vibrational Temperature in 4800–6700-Å System of MnO Molecule

1971 ◽  
Vol 25 (5) ◽  
pp. 554-556
Author(s):  
Prem Shankar Dube ◽  
A. K. Chaudhry ◽  
G. D. Baruah ◽  
D. K. Rai
Keyword(s):  
Electronic Transition ◽  
Vibrational Temperature ◽  
Transition Moment ◽  
Electronic Transition Moment ◽  
Straight Line ◽  
Condon Factors ◽  
Effective Vibrational Temperature ◽  
Franck Condon ◽  
Photographic Photometry

The 4800–6700-Å system of MnO has been excited in an arc. Using the photographic photometry, the relative band intensities have been measured. The data were interpreted with the aid of Franck-Condon factors and r centroids. The electronic transition moment is found to vary according to the relation Re(r) = const (1- 3.192 r + 1.99 r2), where 1.736≤ r≤ 1.90 Å. The slope of the straight line plot of log ∑ v″ I/v4 against G'(ν') for ν' progression gives an estimate of effective vibrational temperature to be 3860 K.

The visible band systems of GeH+ and GeD+ in the helium afterglow

1986 ◽  
Vol 64 (10) ◽  
pp. 1374-1378 ◽  
Author(s):  
Sumio Yamaguchi ◽  
Masaharu Tsuji ◽  
Yukio Nishimura
Keyword(s):  
Electronic Transition ◽  
Transition Moment ◽  
Spectroscopic Constants ◽  
Electronic Transition Moment ◽  
Visible Band ◽  
Condon Factors ◽  
First Time ◽  
Franck Condon ◽  
Morse Potentials ◽  
Higher Sensitivity

The [Formula: see text] intercombination bands of GeH+ and GeD+ have been observed from the helium afterglow reactions of GeH4 and GeD4, respectively. Only the (0,0) band of [Formula: see text] had been rotationally analyzed before; the higher sensitivity of the new measurements made possible the rotational analyses of four weaker bands. Eleven bands of [Formula: see text] were observed for the first time, and rotational analyses were made of five dominant bands. By using isotope relationships, we obtained detailed spectroscopic constants for the [Formula: see text] and X1Σ+ states of GeH+ and GeD+. Franck–Condon factors and r centroids of the [Formula: see text] transitions of GeH+ and GeD+ have been calculated on the basis of Morse potentials. The dependence of the electronic transition moment on the r centroid and the relative vibrational populations of [Formula: see text] and [Formula: see text] have been estimated.

Intensity measurements in emission of 18 Vegard–Kaplan bands of N2

1968 ◽  
Vol 46 (3) ◽  
pp. 221-226 ◽  
Author(s):  
G. Chandraiah ◽  
G. G. Shepherd
Keyword(s):  
Discharge Tube ◽  
Electronic Transition ◽  
Band System ◽  
Internuclear Separation ◽  
Electronic Transition Moment ◽  
Intensity Measurements ◽  
Condon Factors ◽  
Nitrogen Mixture ◽  
Photoelectric Measurements ◽  
Franck Condon

The Vegard–Kaplan band system of nitrogen was excited by running a low-current discharge through a pure xenon–nitrogen mixture contained in a 6-liter spherical bulb of a discharge tube. Photoelectric measurements of the relative intensities of 18 bands (λ 2340–4324 Å) have been made using a 1-m Ebert–Fastie spectrometer. These measured band intensities were used along with Franck–Condon factors qν′ν″ and r centroids [Formula: see text] to study the variation of the electronic transition moment Re(r) with internuclear separation r. It was found that over the measured range from r = 1.23 to 1.43 Å that Re(r) could be represented by[Formula: see text]A "smoothed" set of band strengths [Formula: see text] was determined from this expression for all the observed bands of the Vegard–Kaplan system.

PHOTOELECTRIC INTENSITY MEASUREMENTS UPON BANDS OF THE SiN (B2Σ+−X2Σ+) SPECTRUM

1963 ◽  
Vol 41 (2) ◽  
pp. 240-245 ◽  
Author(s):  
Anne E. Stevens ◽  
H. I. S. Ferguson
Keyword(s):  
Electronic Transition ◽  
Trace Amount ◽  
Transition Moment ◽  
Internuclear Separation ◽  
Electronic Transition Moment ◽  
Intensity Measurements ◽  
Condon Factors ◽  
Microwave Excitation ◽  
Franck Condon

The SiN B2Σ+−X2Σ+ (3800–5200 A) spectrum was excited by continuous introduction of SiCl4 in trace amount into the afterglow produced by microwave excitation of nitrogen. Relative intensities of 21 bands were measured photo-electrically and interpreted with the aid of Franck–Condon factors qν′ν″ and r-centroids [Formula: see text] in terms of the variation of the electronic transition moment Re(r) with internuclear separation r. It was found that Re(r) could be represented empirically by Re(r) = const.(1−1.27r + 0.412r2), [Formula: see text].

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