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Vibronic spectra

Assuming that the PESs are harmonic, the vibrational overlap integral is defined as [Pg.82]

When a normal mode is distorted but is not displaced, then, according to the selection rules, vibronic transitions with odd n, aO — bn , are forbidden. For even n, Franck-Condon factors are expressed as follows  [Pg.82]

As a result, vibronic spectra are less influenced by normal mode distortion than by displacement. [Pg.83]

This section is devoted to the results of ab initio and DFT calculations of PL properties of a variety of point defects in silica nanomaterials, including NBO atoms and their combinations with OVs (Subsection 3.1), silanone and dioxasilyrane defects (Subsection 3.2), and A1 impurity (Subsection 3.3). We demonstrate that the aforementioned defects can give rise to various IR and visible red and green PL bands. [Pg.83]

3 Case Studies Structures and Frequencies of Vinyl Radical in First Three Doublet Excited Electronic States [Pg.129]

Valuable information on the physical-chemical properties of radicals can be often obtained by photoelectron studies in which the electron is detached, so that open-shell systems can be created. Moreover, excited electronic states of radicals can be studied by absorption spectroscopy in the UV-vis regions. An analysis of the resulting experimental spectra can be even more difficult than for ground-state IR or Raman ones. The additional factors can be related to the often not trivial identification of electronic band origin, possible overlap of several electronic transitions and nonadia-batic effects. Although such complications are challenging also for the theoretical approaches, some examples show already their interpretative efficiency. [Pg.129]

TABLE 6.16 Structures, and Adiabatic Excitation (AE) Energies (in eV) of the First Three Doublet Electronic Excited States of the Vinyl Radical. Bond Lengths are in A and Angles in Degrees [Pg.130]

FIGURE 6.6 Vinyl radical plots of the difference in electron density between the ground and the Hrst three doublet excited electronic states. The regions that have lost electron density as a result of the transition are shown in dark blue, and the bright yellow regions gained electron density. [Pg.131]


The first attempt to explain the characteristic properties of molecular spectra in terms of the quantum mechanical equation of motion was undertaken by Born and Oppenheimer. The method presented in their famous paper of 1927 forms the theoretical background of the present analysis. The discussion of vibronic spectra is based on a model that reflects the discovered hierarchy of molecular energy levels. In most cases for molecules, there is a pattern followed in which each electronic state has an infrastructure built of vibrational energy levels, and in turn each vibrational state consists of rotational levels. In accordance with this scheme the total energy, has three distinct components of different orders of magnitude,... [Pg.149]

Fluorescence spectra of pyrene were employed in order to see the polarity of the environment given by the molecular assemblies mentioned so far. The III/I ratio of vibronic spectra of pyrene, a good measure of microenvironmental polarity(194.2Q). is plotted for the DODACl systems as a function of MEGA-n concentrations in Figure 11. [Pg.279]

Recently, the group of Salama has, however, begun to apply the above technique to the study of vibronic spectra of polyacenes that have the dual advantage that they have rather large electron affinities and that they absorb in the near-lR region where alkali atoms, in particular Na, do not absorb. " ... [Pg.823]

Vibronic Spectra of Diatomic Molecules and the Birge-SponerExtrapolation... [Pg.188]

H. Yersin (Ed.), Electronic and Vibronic Spectra of Transition Metal Complexes I, Springer-Verlag, Berlin, 1994. [Pg.1102]

The vibronic transitions in the intraconfigurational dn (crystal-field) transitions have been discussed at length elsewhere (see e.g. Ref. [1]). We concentrate here on new emissions situated in the infrared spectral region and on information from vibronic spectra on distortions in the excited state. [Pg.18]

A well pronounced vibronic spectra is measured from [(CH3)4N]2[IrCl4F2] in which the Ir complex has a geometric trans configuration (cf. Fig. 12) [92,95]. This spectrum is dominated by several charge transfer... [Pg.100]

Electronic and Vibronic Spectra of Transition Metal Complexes I... [Pg.213]

Obtained from Vibronic Spectra and Photon Flux Fluctuation Measured by Time Resolved Spectroscopy... [Pg.23]

The intensity distributions of well resolved vibronic spectra recorded in absorption and emission at low temperature are used to determine the geometric distortions of the electronically excited states of coordination compounds. In particular for complexes of lower symmetry, band analysis is necessary leading to results with which bond distance changes can be calculated. For spectra exhibiting no vibrational fine structure, a new technique is proposed which uses time resolved methods, considering deviations from the Poisson distribution of photons by recording time intervals between two successively emitted photons. [Pg.23]

Vibronic spectra reflect changes in the electronic and vibrational state of a molecule at the same time. It is possible to calculate the geometry of the excited species and the potential hypersurface close to the equilibrium state. For this, a spectrum is required with sufficiently well resolved vibronic structure to carry... [Pg.23]

Vibronic spectra, definition, 23 Visible spectra—See Absorption spectra, Emission spectra... [Pg.276]

In this section, we discuss theoretical methods, which can be applied for calculations of photoabsorption and PL spectra of silica and germania nanoparticles. We start with the choice of model cluster simulating these materials and point defects in them and consider methods for geometry optimization in the ground and excited electronic states (Subsection 2.1). This is followed by the description of more advanced quantum chemical methods for accurate calculations of excitation energies (Subsection 2.2) and the section is completed by the discussion on the theoretical procedure used for predicting vibronic spectra associated with point defects (Subsection 2.3). [Pg.72]

Till recently, computations of vibronic spectra have been limited to small systems or approximated approaches, mainly as a consequence of the difficulties to obtain accurate descriptions of excited electronic states of polyatomic molecules and to computational cost of full dimensional vibronic treatment. Recent developments in electronic structure theory for excited states within the time-dependent density functional theory (TD-DFT) and resolution-of-the-identity approximation of coupled cluster theory (R1-CC2) and in effective approaches to simulate electronic spectra have paved the route toward the simulation of spectra for significantly larger systems. [Pg.134]


See other pages where Vibronic spectra is mentioned: [Pg.512]    [Pg.40]    [Pg.620]    [Pg.366]    [Pg.783]    [Pg.152]    [Pg.169]    [Pg.25]    [Pg.5]    [Pg.6]    [Pg.67]    [Pg.81]    [Pg.81]    [Pg.82]    [Pg.83]    [Pg.15]    [Pg.159]    [Pg.197]    [Pg.106]    [Pg.129]    [Pg.129]    [Pg.131]    [Pg.133]    [Pg.133]    [Pg.134]    [Pg.135]   
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See also in sourсe #XX -- [ Pg.406 , Pg.419 ]

See also in sourсe #XX -- [ Pg.176 ]




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