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Electron transitions for

Figure 5. Ground-state conflguration and configurations corresponding formally to one-electron transitions for a system having one unpaired electron in its ground state. Figure 5. Ground-state conflguration and configurations corresponding formally to one-electron transitions for a system having one unpaired electron in its ground state.
A schematic molecular orbital diagram for the Fe-Fe interaction in an S = I valence-delocalized Fe Fe pair based on effective C v symmetry at the Fe sites and the observed electronic transitions for the valance-delocalized [Fe2S2l cluster is shown in Fig. 15. The dominant interaction (responsible for the S = ground state) is the a overlap between the pair of orbitals, with progressively smaller tt interactions between pairs of d z and dyz orbitals and S interactions between pairs of d y amd / orbitals. The three highest energy tran-... [Pg.45]

Figure 1.5. Localized molecular orbitals formed from the atomic basis orbitals and electronic transitions for the carbonyl group. Figure 1.5. Localized molecular orbitals formed from the atomic basis orbitals and electronic transitions for the carbonyl group.
Figure 5.1. Potential energy diagram depicting electron transition for an excimer laser having an emission at 248 nm (from Pummer41). Figure 5.1. Potential energy diagram depicting electron transition for an excimer laser having an emission at 248 nm (from Pummer41).
Tab. 7.5 Ultraviolet-visible absorption bands and electron transitions for the iron oxides (data for magnetite, A/ustite and akaganeite from Strens Wood, 1979 A/ith permission bernalite from McCammon et al.,1995 remainder from Sherman Waite, 1985 A/ith permission)... Tab. 7.5 Ultraviolet-visible absorption bands and electron transitions for the iron oxides (data for magnetite, A/ustite and akaganeite from Strens Wood, 1979 A/ith permission bernalite from McCammon et al.,1995 remainder from Sherman Waite, 1985 A/ith permission)...
There is one other means of determining lifetime, available if both photo-Hall (PH) and absorption experiments can be carried out. This possibility is simply illustrated by Eq. (35). Here the PH measurement gives An, the absorption measurement gives ocB, and f0 can be easily measured with a calibrated light detector. An obvious caveat here, of course, is that we must assume that a = aB, i.e., that all of the light absorption is due to electronic transitions. For above-band-gap light this assumption will almost certainly be true. It was seen before that absorption measurements can be useful in determining impurity concentrations. Thus, a combination of PH and absorption data may yield both N and rB. If the carrier mobility can... [Pg.126]

Figure 1.4 Diagram of energy levels and electronic transitions for atomic sodium. Figure 1.4 Diagram of energy levels and electronic transitions for atomic sodium.
First of all, what types of energies are there For a monatomic, inert gas at ordinary temperatures we need only consider the kinetic energy due to the translational motion. That is, we do not need to consider nuclear reactions or electronic transitions, for example. [Pg.338]

The electronic transition for a molecule from G to Sv represented by the vertical arrow in Figure 5.3, has a high probability of occurring if the energy of the photon corresponds to the energy necessary to promote an electron from energy level E to energy level E2 ... [Pg.143]

The Einstein coefficients are related to the most fundamental quantity which describes the transition probability, known as the transition moment. During an electronic transition for instance, an electron jumps from one orbital to another. Its distance from the nucleus changes, so there is a change in the instantaneous dipole moment. The greater this change, the more probable the transition because it is the interaction between this transition dipole and the electric vector of light. [Pg.23]

A complex 7THG can result from one-, two-, or three-photon resonances. One-photon resonance occurs when the fundamental frequency co is close to an allowed electronic transition. Two-photon resonance occurs when 2co is close to a two-photon allowed electronic transition. For centrosymmetric molecules the two-photon selection rule couples states of like inversion symmetry, e.g. g <- g. For acentric molecules one-photon transitions can also be two-photon allowed. Three-photon resonance occurs when 3co is close to the energy of an electronic transition the same symmetry rules apply as for one-photon transitions. [Pg.88]

We consider two electronic transitions for each guanine and adenine chro-mophore and one for each cytosine and thymine chromophore. The dipolar coupling among all the pairs of the thirty transitions was considered and... [Pg.130]

The C-17 side-chain of corticosteroids does not contain a chromophoric group suitable for spectrophotometric measurement, nor does oxidation of the chain lead directly to spectrophotometrically active derivatives. However, the 20-keto group of the 17 a-ketol side-chain, as a chirally perturbed chromophoric group, has an optically active absorbance band in the interval 270-300 nm that is characteristic of the n-7T electronic transition for saturated ketones. An intense positive Cotton effect is observed in the CD spectra see the CD spectra for hydrocortisone and cortisone in Figures 8 and 9. [Pg.302]

With reference to absorption spectroscopy, we deal here with photon absorption by electrons distributed within specific orbitals in a population of molecules. Upon absorption, one electron reaches an upper vacant orbital of higher energy. Thus, light absorption would induce the molecule excitation. Transition from ground to excited state is accompanied by a redistribution of an electronic cloud within the molecular orbitals. This condition is implicit for transitions to occur. According to the Franck-Condon principle, electronic transitions are so fast that they occur without any change in nuclei position, that is, nuclei have no time to move during electronic transition. For this reason, electronic transitions are always drawn as vertical lines. [Pg.1]

Figure 3.1 Electronic transitions for an octahedral transition metal complex. LC, ligand centred LMCT, ligand-to-metal charge transfer MC, metal centred MLCT, metal-to-ligand charge transfer... Figure 3.1 Electronic transitions for an octahedral transition metal complex. LC, ligand centred LMCT, ligand-to-metal charge transfer MC, metal centred MLCT, metal-to-ligand charge transfer...
This raised the problem of finding the probabilities of the excitations of the many-atomic valine molecule (64 electrons) caused by the j8 decay of a tritium nucleus. Earlier, the influence of the tritium / decay on the electron shell excitations was studied only for the simplest molecules. The most precise calculations were performed for HT by Wolniewicz (1965). However, the considered transitions were only those into the ground and the first excited states of HHe+. A number of selected electron transitions for molecules OHT, NH2T, and CH3T were calculated by Ikuta et al. (1977). A consistent analysis of all the aspects of the influence of ft decay on the electron shell rearrangement for different types of molecules was performed by Kaplan et al., (1982, 1983), who have also calculated the distribution of excitation probabilities and the / spectrum of the tritium-containing valine. [Pg.292]

For this study we have used methylen-cyclopropene (MCP) and acrolein (ACRO) in two solvents, an apolar (dioxane) and a polar one (acetonitrile). The selected transitions can be seen as representative examples of different types of electronic transitions for which different solvent responses can be studied for MCP the first 77 - 77 transition for MCP, and the first n -> 77 and 77 -> 77 transitions for ACRO. We note that in MCP the resulting excited state is characterized by a dipole moment which has an opposite direction with respect to that of the ground state, whereas in ACRO, the n -> 77 and 77 -> 77 transitions are characterized by a decrease and an increase in the dipole moment passing from ground to excited state, respectively. [Pg.198]

Figure 7 Electronic states, their charge, spin state, and the corresponding electronic transitions for (a) solitons (b) polarons and (c) bipolarons. Figure 7 Electronic states, their charge, spin state, and the corresponding electronic transitions for (a) solitons (b) polarons and (c) bipolarons.

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Electron Orbital Assignments for Some Transition Elements

Electronic transitions responsible for

Exact selection rules for electronic transitions

Notation Schemes for Electronic Transitions

Selection rules for electronic transitions

Spectroscopic Techniques for Measuring Collision-Induced Transitions in the Electronic Ground State of Molecules

The 18-Electron Rule for Transition Metal Bonding

The Selection Rules for Electronic Transitions

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