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Energy levels anharmonic oscillator

Figure 2. Working diagram showing how the linear free-energy relationship, common in electrode process kinetics, arises from changes in electrode potential. is a symmetry factor. An extreme case of an anharmonic oscillator energy profile is shown in schematic form (cf. Ref. 25). This representation assumes changes in V affect only the energy of electrons in the initial state at the Fermi level. Figure 2. Working diagram showing how the linear free-energy relationship, common in electrode process kinetics, arises from changes in electrode potential. is a symmetry factor. An extreme case of an anharmonic oscillator energy profile is shown in schematic form (cf. Ref. 25). This representation assumes changes in V affect only the energy of electrons in the initial state at the Fermi level.
D. G. Truhlar, Oscillators with quartic anharmonicity Approximate energy levels,/. Molec. Spec. 38 4151 (1971). [Pg.379]

The Morse oscillator energy levels are expressed in terms of a single parameter, a, the anharmonicity constant as... [Pg.185]

The other approach for finding the anharmonic corrections for the quantum Morse oscillator models involves performing a direct count of the vibrational energy levels, with the Morse oscillator energy levels given by ... [Pg.537]

These harmonic-oscillator solutions predict evenly spaced energy levels (i.e., no anharmonicity) that persist for all v. It is, of course, known that molecular vibrations display anharmonicity (i.e., the energy levels move closer together as one moves to higher v) and that quantized vibrational motion ceases once the bond dissociation energy is reached. [Pg.69]

The reason that does not change with isotopic substitution is that it refers to the bond length at the minimum of the potential energy curve (see Figure 1.13), and this curve, whether it refers to the harmonic oscillator approximation (Section 1.3.6) or an anharmonic oscillator (to be discussed in Section 6.1.3.2), does not change with isotopic substitution. Flowever, the vibrational energy levels within the potential energy curve, and therefore tq, are affected by isotopic substitution this is illustrated by the mass-dependence of the vibration frequency demonstrated by Equation (1.68). [Pg.132]

Figure 6.4 Potential energy curve and energy levels for a diatomic molecule behaving as an anharmonic oscillator compared with those for a harmonic oscillator (dashed curve)... Figure 6.4 Potential energy curve and energy levels for a diatomic molecule behaving as an anharmonic oscillator compared with those for a harmonic oscillator (dashed curve)...
Two of the most severe limitations of the harmonic oscillator model, the lack of anharmonicity (i.e., non-uniform energy level spacings) and lack of bond dissociation, result from the quadratic nature of its potential. By introducing model potentials that allow for proper bond dissociation (i.e., that do not increase without bound as x=>°°), the major shortcomings of the harmonic oscillator picture can be overcome. The so-called Morse potential (see the figure below)... [Pg.36]

To obtain the allowed energy levels, Ev, for a real diatomic molecule, known as an anharmonic oscillator, one substitutes the potential energy function describing the curve in Fig. 3.2c into the Schrodinger equation the allowed energy levels are... [Pg.44]

When exposed to electromagnetic radiation of the appropriate energy, typically in the infrared, a molecule can interact with the radiation and absorb it, exciting the molecule into the next higher vibrational energy level. For the ideal harmonic oscillator, the selection rules are Av = +1 that is, the vibrational energy can only change by one quantum at a time. However, for anharmonic oscillators, weaker overtone transitions due to Av = +2, + 3, etc. may also be observed because of their nonideal behavior. For polyatomic molecules with more than one fundamental vibration, e.g., as seen in Fig. 3.1a for the water molecule, both overtones and... [Pg.44]

In the LM model, molecular vibrations are treated as motions of individual anharmonic bonds [38] (usually Morse oscillators). They therefore include anharmonicity, but not coupling between bonds, thus requiring inclusion of interbond coupling for obtaining a better description. For the case of t identical Morse oscillators, the energy levels related to the LM Hamiltonian are given by... [Pg.29]

Energy levels in the anharmonic oscillator are not equal, although they become slightly closer as energy increases. This phenomenon can be seen in the following equation , ... [Pg.373]

S. E. Stein and B. S. Rabinovitch. Accurate Evaluation of Internal Energy Level Sums and Densities Including Anharmonic Oscillators and Hindered Rotors. J. Chem. Phys., 58 2438-2445,1973. [Pg.836]

Theory predicts that for a harmonic oscillator only a change from one vibrational energy level to the next higher is allowed, but for anharmonic oscillators weaker transitions to higher vibrational energy levels can occur. The resulting "overtones" are found at approximate multiples of the frequency of the fundamental. Combination frequencies representing sums... [Pg.1277]

In the lowest order of perturbation theory, the energy levels of the three-dimensional anharmonic oscillator are... [Pg.247]

Although the vibrational motion of a diatomic molecule conforms quite closely to that of a harmonic oscillator, in practice the anharmonic deviations are quite significant and must be taken into account if vibrational energy levels are to be modelled accurately. A general form of the potential fimction V in equation (2.157) was proposed by Dunham... [Pg.65]

If there was no interaction between vibration and rotation, the energy levels would be given by the simple sum of the expression giving the vibrational levels for the anharmonic oscillator, equation (6.188), and that describing the rotational levels of the rigid rotor, equation (6.162). There is an interaction, however during a vibration the moment of inertia of the molecule changes, and therefore so also does the rotational constant. We may therefore use a mean value of Bv for the rotational constant of the vibrational level considered, i.e. [Pg.243]

Figure 13 Energy level scheme for a system of two coupled oscillators. The isolated peptide states (left side) are coupled by some weak interaction, which mixes them to generate the excitonic states (right side). Anharmonicity, which is crucial for understanding the 2D pump probe spectra, is introduced into this model by lowering the energies of the double excited monomeric site states i2) and j2) by A from their harmonic energies 2eu- This anharmonicity mixes into all coupled states, giving rise to diagonal anharmonicity (Ae ) and off-diagonal anharmonicity (mixed-mode anharmonicity, Ae i) in the basis of the normal modes discussed in the text. Figure 13 Energy level scheme for a system of two coupled oscillators. The isolated peptide states (left side) are coupled by some weak interaction, which mixes them to generate the excitonic states (right side). Anharmonicity, which is crucial for understanding the 2D pump probe spectra, is introduced into this model by lowering the energies of the double excited monomeric site states i2) and j2) by A from their harmonic energies 2eu- This anharmonicity mixes into all coupled states, giving rise to diagonal anharmonicity (Ae ) and off-diagonal anharmonicity (mixed-mode anharmonicity, Ae i) in the basis of the normal modes discussed in the text.

See other pages where Energy levels anharmonic oscillator is mentioned: [Pg.49]    [Pg.847]    [Pg.25]    [Pg.144]    [Pg.240]    [Pg.703]    [Pg.82]    [Pg.79]    [Pg.113]    [Pg.92]    [Pg.133]    [Pg.381]    [Pg.526]    [Pg.51]    [Pg.260]    [Pg.251]    [Pg.380]    [Pg.301]    [Pg.108]    [Pg.144]    [Pg.240]    [Pg.11]    [Pg.426]    [Pg.6370]    [Pg.39]    [Pg.40]   
See also in sourсe #XX -- [ Pg.417 , Pg.438 ]




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