Research Article

THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE

Volume: 31 January 1, 1985
  • A. Abdel-rahman
EN

THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE

Abstract

The geometry of the SCC12 molecule in the electronic excited State, JA2 -> ’A^ has been determined using the polydimentional Franck-Condon method. The molecule in the ground electronic State is plannar and belongs to the C2V point group, while in the excited State in beco- mes non-plannar and changes symmetry to the .C point group. This change in symmetry is ac- companied by the increase of the values of the molecular dimensions compared with those in the ground State, increase in the in C = S, C —- C1 bond lengths and in C1CC1 angle are evalu- ated to be 0.1838, 0.06845 Â and 9.01°, reöpectively.

Keywords

References

  1. Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering

Details

Primary Language

English

Subjects

Chemical Engineering

Journal Section

Research Article

Authors

A. Abdel-rahman This is me
Türkiye

Publication Date

January 1, 1985

Submission Date

January 1, 1985

Acceptance Date

-

Published in Issue

Year 1985 Volume: 31

APA
Abdel-rahman, A. (1985). THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE. Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering, 31. https://doi.org/10.1501/Commub_0000000275
AMA
1.Abdel-rahman A. THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE. Commun. Fac. Sci. Univ. Ank. Ser. B. 1985;31. doi:10.1501/Commub_0000000275
Chicago
Abdel-rahman, A. 1985. “THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE”. Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering 31 (January). https://doi.org/10.1501/Commub_0000000275.
EndNote
Abdel-rahman A (January 1, 1985) THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE. Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering 31
IEEE
[1]A. Abdel-rahman, “THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE”, Commun. Fac. Sci. Univ. Ank. Ser. B, vol. 31, Jan. 1985, doi: 10.1501/Commub_0000000275.
ISNAD
Abdel-rahman, A. “THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE”. Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering 31 (January 1, 1985). https://doi.org/10.1501/Commub_0000000275.
JAMA
1.Abdel-rahman A. THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE. Commun. Fac. Sci. Univ. Ank. Ser. B. 1985;31. doi:10.1501/Commub_0000000275.
MLA
Abdel-rahman, A. “THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE”. Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering, vol. 31, Jan. 1985, doi:10.1501/Commub_0000000275.
Vancouver
1.A. Abdel-rahman. THE FRANCK-CONDON PRINC1PLE AND THE GEOMETRY OF SCCI2 IN THE EXCITED ELECTRONIC STATE. Commun. Fac. Sci. Univ. Ank. Ser. B. 1985 Jan. 1;31. doi:10.1501/Commub_0000000275

Communications Faculty of Sciences University of Ankara Series B Chemistry and Chemical Engineering

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