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Energy levels 274 Subject

Fig. 1. Symmetric double-well potential U-(Q) for a pseudo-JT molecule with two nondegenerate electronic terms coupled to one low-symmetry mode [equation (9)]. The curve corresponds to strong coupling case with k = 4 and a relatively large energy gap, A = 12 (both in units of hcS). The dashed line represents the twofold degenerate ground-state energy level subject to a tunneling splitting. Fig. 1. Symmetric double-well potential U-(Q) for a pseudo-JT molecule with two nondegenerate electronic terms coupled to one low-symmetry mode [equation (9)]. The curve corresponds to strong coupling case with k = 4 and a relatively large energy gap, A = 12 (both in units of hcS). The dashed line represents the twofold degenerate ground-state energy level subject to a tunneling splitting.
When subjected to an electron bombardment whose energy level is much higher than that of hydrocarbon covalent bonds (about 10 eV), a molecule of mass A/loses an electron and forms the molecular ion, the bonds break and produce an entirely new series of ions or fragments . Taken together, the fragments relative intensities constitute a constant for the molecule and can serve to identify it this is the basis of qualitative analysis. [Pg.48]

The Boltzmann distribution is fundamental to statistical mechanics. The Boltzmann distribution is derived by maximising the entropy of the system (in accordance with the second law of thermodynamics) subject to the constraints on the system. Let us consider a system containing N particles (atoms or molecules) such that the energy levels of the... [Pg.361]

Consider what happens if, for example, an ensemble of carbon atoms is subjected to X rays of 1486.6 eV energy (the usual X-ray source in commercial XPS instruments). A carbon atom has 6 electrons, two each in the Is, 2s, and 2p orbitals, usually written as C Is 2s 2p. The energy level diagram of Figure la represents this electronic structure. The photoelectron process for removing an electron from the... [Pg.284]

The steric environment of the atoms in the vicinity of the reaction centre will change in the course of a chemical reaction, and consequently the potential energy due to non-bonded interactions will in general also change and contribute to the free energy of activation. The effect is mainly on the vibrational energy levels, and since they are usually widely spaced, the contribution is to the enthalpy rather than the entropy. When low vibrational frequencies or internal rotations are involved, however, effects on entropy might of course also be expected. In any case, the rather universal non-bonded effects will affect the rates of essentially all chemical reactions, and not only the rates of reactions that are subject to obvious steric effects in the classical sense. [Pg.2]

Figure 4.2 Energy levels and populations for an IS system in which nuclei I and S are not directly coupled with each other. This forms the basis of the nuclear Overhauser enhancement effect. Nucleus S is subjected to irradiation, and nucleus I is observed, (a) Population at thermal equilibrium (Boltzmann population). Figure 4.2 Energy levels and populations for an IS system in which nuclei I and S are not directly coupled with each other. This forms the basis of the nuclear Overhauser enhancement effect. Nucleus S is subjected to irradiation, and nucleus I is observed, (a) Population at thermal equilibrium (Boltzmann population).
In the solid, electrons reside in the valence band but can be excited into the conduction band by absorption of energy. The energy gap of various solids depends upon the nature of the atoms comprising the solid. Semiconductors have a rather narrow energy gap (forbidden zone) whereas that of insulators is wide (metals have little or no gap). Note that energy levels of the atoms "A" are shown in the valence band. These will vary depending upon the nature atoms present. We will not delve further into this aspect here since it is the subject of more advanced studies of electronic and optical materieds. [Pg.41]

The position of energy level is subjected to fluctuations, whereas that of level 8 is independent of solvent polarization. [Pg.647]

A further technique exists for the determination of triplet energy levels. This technique, called electron impact spectroscopy, involves the use of inelastic scattering of low-energy electrons by collision with molecules. The inelastic collisions of the electrons with the molecules result in transfer of the electron energy to the molecule and the consequent excitation of the latter. Unlike electronic excitation by photons, excitation by electron impact is subject to no spin selection rule. Thus transitions that are spin and/or orbitally forbidden for photon excitation are totally allowed for electron impact excitation. [Pg.117]

Energy levels within an atom or molecule can be populated in several ways to produce more target species in the higher energy excited state than in the ground state. The population can occur by collisional processes such as between molecules in the interstellar medium and a balance can occur between the excitation process and a number of deactivation processes (Figure 3.17a). The population of level 2 can be subjected to ... [Pg.77]

All forms of energy are subject to the rules of quantum mechanics, which allow only certain (discrete) energy levels to exist. Therefore, an isolated molecule cannot contain... [Pg.126]

The content of The Forces Between Molecules, by Maurice Rigby, E. Brian Smith, William A. Wakeham and Geoffrey C. Maitland, Oxford University Press, Oxford, 1986, is more explicitly about interactions than formal bonds. Again, it will be a fairly austere and mathematical read. In the Oxford Primer series, try Energy Levels in Atoms and Molecules by W. G. Richards and P. R. Scott, Oxford University Press, Oxford, 1994. It s easier than the two books above, and again helps provide some of the background material to the subject. It is still mathematically based. [Pg.538]

Characterizing the performance of the OLED devices requires an understanding of how the device functions and how the performance is measured. First, we discuss the subjective visual response in relation to the objective emission of light. Then we describe basic measurements and efficiency calculations. Next, we describe energy levels in OLED devices. Finally, we discuss the lifetime measurements. [Pg.624]


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