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Harmonic oscillators spectroscopy

Infrared (ir) transmission depends on the vibrational characteristics of the atoms rather than the electrons (see Infrared and Raman spectroscopy). For a diatomic harmonic oscillator, the vibrational frequency is described by... [Pg.332]

The vibrational and rotational motions of the chemically bound constituents of matter have frequencies in the IR region. Industrial IR spectroscopy is concerned primarily with molecular vibrations, as transitions between individual rotational states can be measured only in IR spectra of small molecules in the gas phase. Rotational - vibrational transitions are analysed by quantum mechanics. To a first approximation, the vibrational frequency of a bond in the mid-IR can be treated as a simple harmonic oscillator by the following equation ... [Pg.311]

Presented below are three examples designed to give the reader some idea of what one can expect from the theoretical analysis of vibrational spectra based on the simple harmonic oscillator model. Systems have been chosen whose structures have been know for many years and, in fact, were known prior to the availability of IR spectroscopy. Hence their spectra have previously been well characterized and these serve as a test of the method . [Pg.156]

Figure 9.7 Vibrational energy levels determined from solution of the one-dimensional Schrodinger equation for some arbitrary variable 6 (some higher levels not shown). In addition to the energy levels (horizontal lines across the potential curve), the vibrational wave functions are shown for levels 0 and 3. Conventionally, the wave functions are plotted in units of (probability) with the same abscissa as the potential curve and an individual ordinate having its zero at the same height as the location of the vibrational level on the energy ordinate - those coordinate systems are explicitly represented here. Note that the absorption frequency typically measured by infrared spectroscopy is associated with the 0 —> 1 transition, as indicated on the plot. For the harmonic oscillator potential, all energy levels are separated by the same amount, but this is not necessarily the case for a more general potential... Figure 9.7 Vibrational energy levels determined from solution of the one-dimensional Schrodinger equation for some arbitrary variable 6 (some higher levels not shown). In addition to the energy levels (horizontal lines across the potential curve), the vibrational wave functions are shown for levels 0 and 3. Conventionally, the wave functions are plotted in units of (probability) with the same abscissa as the potential curve and an individual ordinate having its zero at the same height as the location of the vibrational level on the energy ordinate - those coordinate systems are explicitly represented here. Note that the absorption frequency typically measured by infrared spectroscopy is associated with the 0 —> 1 transition, as indicated on the plot. For the harmonic oscillator potential, all energy levels are separated by the same amount, but this is not necessarily the case for a more general potential...
In vibrational spectroscopy, where the treatment of molecular vibrations is based on the differential equation for an harmonic oscillator ... [Pg.139]

Slater s theory assumes that the normal modes behave as harmonic oscillators, which requires that there be no flow of energy between the normal modes once the molecule is suitably activated, and so the energy distribution remains fixed between collisions. But spectroscopy shows that energy can flow around a molecule, and allowing for such a flow between collisions vastly improves the theory. Like Kassel s theory a fully quantum theory would be superior. [Pg.161]

The polyad quantum number is defined as the sum of the number of nodes of the one-electron orbitals in the leading configuration of the Cl wave function [19]. The name polyad originates from molecular vibrational spectroscopy, where such a quantum number is used to characterize a group of vibrational states for which the individual states cannot be assigned by a set of normal-mode quantum numbers due to a mixing of different vibrational modes [19]. In the present case of quasi-one-dimensional quantum dots, the polyad quantum number can be defined as the sum of the one-dimensional harmonic-oscillator quantum numbers for all electrons. [Pg.184]

Surprisingly, the enthalpy of combustion of isoxazole was determined only very recently.270 For isoxazole, AH° (298.15 K) = —(394.70 + 0.12) kcalth mol-1, from which the enthalpy of formation in the gas phase was derived as AHf (g) = 18.78 0.13 kcalth mol-1. The enthalpies of combustion of 3-amino-5-methylisoxazole and 5-amino-3,4-dimethylisoxazole have also been determined.271 Thermodynamic parameters for isoxazole have been derived from vibrational spectra using the harmonic oscillator-rigid rotor approximation.272,273 Analysis of the rotational spectra of isotopic forms of isoxazole, studied by double resonance modulated microwave spectroscopy, has given the molecular dimensions shown in Fig. 1.274,275... [Pg.199]

In order to investigate solids or polymer systems with free carriers by IR spectroscopy, it is very convenient to measure the reflectivity instead of absorbance or transmittance. Thus, the problems to be discussed in this context are usually described by a linear response formalism. In its simplest form, this means that the response function (dielectric function) s(u ) of a damped harmonic oscillator is used to describe the interaction between light and matter. The complex form of this function is... [Pg.374]

The simplest system that can be studied by vibrational spectroscopy is the diatomic molecule, and the simplest model for its vibration is the harmonic oscillator. If the atoms have masses m, and and are connected by an ideal spring, at rest they have an equilibrium separation and on extension or compression (rg Ar) the masses are subject to a restoring force proportional to the displacement ... [Pg.50]

The theoretical background which will be needed to calculate the excited state distortions from electronic and Raman spectra is discussed in this section. We will use the time-dependent theory because it provides both a powerful quantitative calculational method and an intuitive physical picture [42,46-50]. The method shows in a simple way the inter-relationship between Raman and electronic spectroscopy. It demonstrates that the intensity of a peak in a resonance Raman spectrum provides detailed information about the displacement of the excited state potential surface along the normal mode giving rise to the peak [42,48]. It can also be used to calculate distortions from the intensities of vibronic peaks in electronic spectra [49]. For harmonic oscillators, the time-dependent theory is mathematically equivalent to the familiar Franck-Condon calculation [48]. [Pg.129]

The harmonic oscillator model enables measurement of the bond force constant through vibrational spectroscopy as follows. The measured frequency of the radiation absorbed is the same as the vibrational frequency of the molecule. The reduced mass is calculated for the molecule, and the force constant is evaluated as k =... [Pg.161]

Section 4.7 introduces the quantum harmonic oscillator and provides the groundwork for subsequent discussions of vibrational spectroscopy. This section is completely new. [Pg.1083]

Vibrational dynamics are dominantly represented with normal modes that are coherent harmonic oscillations of all degrees of freedom at the same frequency [Wilson 1964 Califano 1981 Long 2002 Ferraro 2003], In the classical regime, normal coordinates - the eigenvectors of the dynamical matrix -are determined only to an arbitrary proportionality factor. In other words, the effective mass associated to a normal mode is arbitrary. This is of no consequence for optical spectroscopy techniques (infrared and Raman) that cannot probe masses, because of tiny momentum transfer values. Only recently, effective masses have been determined thanks to vibrational spectroscopy with neutrons [Ikeda 2002], The existence of well-defined (of course) effective masses should be included in further theoretical developments. [Pg.504]

The textbook case of the harmonic oscillator in one dimension with mass m presented in this section is meant to feature neutron scattering experiments, compared to infrared and Raman spectroscopy. The Hamiltonian... [Pg.506]

The definition of a theory as a set of hypotheses that has passed a test of experimental verification is uncontroversial. However, the equation of theories and models proposed by Zumdahl and Petrucci and Harwood is less straightforward, I think. It surely is true that all but the most grandiose of scientists would admit that their theories were approximations to reality, and so, to the extent that a model requires a specified list of approximations, all theories are models. However, not all models are theories. If I make the approximation of treating molecules as perfect spheres or springs as massless, I am creating a model that will make subsequent calculation easier or comprehension of the results easier, but I presumably do not believe these approximations to be true in my theory of what is occurring in reality. Chemists will talk of the harmonic-oscillator model as a mathematically convenient approximation for the interpretation of vibrational spectra, but I do not think many people would consider this to be a theory of vibrational spectroscopy. [Pg.215]

We now we summarize some of the procedures that are used in analyzing multidimensional IR data. Constants factors are often omitted from the formulas as are the transition dipole factors which are easily incorporated [74] when the modes are a collection of coupled harmonic oscillators. More generally the variations of transition dipole with nuclear displacement should be incorporated. It is often useful to compare the 2D-IR results with the results of other nonlinear experiments because it turns out that various manipulations of these multidimensional signals provide all of the common nonlinear results such as echoes, gratings, degenerate four wave effects, and pump-probe spectroscopy. [Pg.19]

Fairly good agreement exists between the calculated value of 1682 cm-1 and the experimental value of 1650 cm1. Direct correlation does not exist because Hooke s law assumes that the vibrational system is an ideal harmonic oscillator and, as mentioned before, the vibrational frequency for a single chemical moiety in a polyatomic molecule corresponds to the vibrations from a group of atoms. Nonetheless, based on the Hooke s law approximation, numerous correlation tables have been generated that allow one to estimate the characteristic absorption frequency of a specific functionality (13). It becomes readily apparent how IR spectroscopy can be used to identify a molecular entity, and subsequently physically characterize a sample or perform quantitative analysis. [Pg.520]

A related measure of the intensity often used for electronic spectroscopy is the oscillator strength,/ This is a dimensionless ratio of the transition intensity to that expected for an electron bound by Hooke s law forces so as to be an isotropic harmonic oscillator. It can be related either to the experimental integrated intensity or to the theoretical transition moment integral ... [Pg.1126]


See other pages where Harmonic oscillators spectroscopy is mentioned: [Pg.69]    [Pg.205]    [Pg.5]    [Pg.24]    [Pg.368]    [Pg.227]    [Pg.236]    [Pg.93]    [Pg.171]    [Pg.93]    [Pg.323]    [Pg.100]    [Pg.156]    [Pg.499]    [Pg.116]    [Pg.173]    [Pg.283]    [Pg.24]    [Pg.314]    [Pg.113]    [Pg.165]    [Pg.116]    [Pg.152]    [Pg.4746]   


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