ANALYTIC POTENTIAL FUNCTIONS FOR DIATOMIC MOLECULES [electronic resource] : SOME LIMITATIONS
- Published:
- Berkeley, Calif. : Lawrence Berkeley National Laboratory, 1979.
Oak Ridge, Tenn. : Distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy. - Additional Creators:
- Lawrence Berkeley National Laboratory and United States. Department of Energy. Office of Scientific and Technical Information
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- Restrictions on Access:
- Free-to-read Unrestricted online access
- Summary:
- In discussions of the spectra of diatomic molecules, it is common in many physical chemistry and spectroscopy texts to introduce the Morse potential function V(R) = D{sub e}(1-exp(-β(R-R{sub e}))) as representative of the real potential. The length scaling factor, β, is usually expressed in terms of the harmonic vibration constant, ω{sub e}, the molecular reduced mass, μ, and the well depth, D{sub e}, via β = k ω{sub e}(2π²μ/D{sub e}){sup 1/2} where k is a collection of physical constants appropriate to the units used for ω{sub e}, d{sub e}, μ, and β. The Morse potential has the advantage that many simple, analytical expressions, such as eqn. (2), exist among the parameters of the potential function and observable spectroscopic constants.
- Report Numbers:
- E 1.99:lbl-10171
lbl-10171 - Subject(s):
- Other Subject(s):
- Note:
- Published through SciTech Connect.
11/01/1979.
"lbl-10171"
Journal of Chemical Education FT
Winn, John S.
Materials Sciences Division - Funding Information:
- DE-AC02-05CH11231
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