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Field Effect Theory

It is obvious that no theory of the extrinsic field effect can be developed without a good understanding of conversion theory for the nondissocia-tive process in the absence of an applied magnetic field. The status of k0 calculations for various systems has been reviewed many times and will be summarized very briefly here. The original development by Wigner [Pg.50]

Understanding the several extrinsic field effects has proved to be difficult because of our failure, in more than a few cases, to identify the [Pg.51]

This review will be concluded with some speculative remarks on possible sources of the several extrinsic field effects. There is one kind of behavior that appears to have a simple explanation. The ferromagnetic catalysts all show zero field effect below Tc The reason for this must be that in all such substances the Weiss molecular field is of the order of 10s to 107 Oe. An extrinsic field of a few kOe could produce little additional effect. [Pg.54]

Evidence pointing to the existence of k+ and kr sites will be reviewed  [Pg.54]

For k+ sites Ak tends to become independent of field above 104 Oe. On k sites saturation occurs at below 102 Oe. [Pg.55]


Karlberg GS, Rossmeisl J, Nprskov JK. 2007b. Estimations of electric field effects on the oxygen reduction reaction based on the density functional theory. Phys Chem Chem Phys 37 5158-5161. [Pg.89]

In this paper a method [11], which allows for an a priori BSSE removal at the SCF level, is for the first time applied to interaction densities studies. This computational protocol which has been called SCF-MI (Self-Consistent Field for Molecular Interactions) to highlight its relationship to the standard Roothaan equations and its special usefulness in the evaluation of molecular interactions, has recently been successfully used [11-13] for evaluating Eint in a number of intermolecular complexes. Comparison of standard SCF interaction densities with those obtained from the SCF-MI approach should shed light on the effects of BSSE removal. Such effects may then be compared with those deriving from the introduction of Coulomb correlation corrections. To this aim, we adopt a variational perturbative valence bond (VB) approach that uses orbitals derived from the SCF-MI step and thus maintains a BSSE-free picture. Finally, no bias should be introduced in our study by the particular approach chosen to analyze the observed charge density rearrangements. Therefore, not a model but a theory which is firmly rooted in Quantum Mechanics, applied directly to the electron density p and giving quantitative answers, is to be adopted. Bader s Quantum Theory of Atoms in Molecules (QTAM) [14, 15] meets nicely all these requirements. Such a theory has also been recently applied to molecular crystals as a valid tool to rationalize and quantitatively detect crystal field effects on the molecular densities [16-18]. [Pg.105]

Equation (96) shows that the effective KS potential may be simply obtained by adding to the standard KS potential of the isolated solute, an electrostatic correction which turns out to be the RE potential Or, and the exchange- correlation correction 8vxc. It is worth mentioning here, that Eq (96) is formally equivalent to the effective Fock operator correction bfteffi defined in the context of the self consistent reaction field (SCRF) theory [2,3,14] within the HF theory, the exchange contribution is exactly self-contained in Or, whereas correlation effects are completely neglected. As a result, within the HF theory 8v = Or, as expected. [Pg.115]

Angyan, J. G. Choosing between alternative MP2 algoritms in the selfconsistent reaction field (SCRF) theory of solvent effects, Chem.Phys.Lett., in press (1995),... [Pg.352]

From our experimental results and different models used in theoretical calculations using either CND0/2 (23-25, 37>38) and PCIL0 methods (26,27), or the electric field effect by IND0 finite perturbation theory (28), the following models can be supposed ... [Pg.106]

Abstract The equation of state (EOS) of nuclear matter at finite temperature and density with various proton fractions is considered, in particular the region of medium excitation energy given by the temperature range T < 30 MeV and the baryon density range ps < 1014 2 g/cm3. In this region, in addition to the mean-field effects the formation of few-body correlations, in particular light bound clusters up to the alpha-particle (1 < A < 4) has been taken into account. The calculation is based on the relativistic mean field theory with the parameter set TM1. We show results for different values for the asymmetry parameter, and (3 equilibrium is considered as a special case. [Pg.75]

To construct the low energy effective theory of the fermionic system, we rewrite the fermion fields as... [Pg.178]

The two above features which modify the simplest theory extend the range of distances z between the fluorophore and the surface over which the results remain valid, from a minimum of several hundred nanometers without the modifications to less than ten nanometers with them. Those two features are incorporated into the results displayed here. Other refinements, not included here, involve consideration of energy transfer to electron-hole pairs (for metals only at z < 10 nm) and nonhomogeneous atomic field effects (z<0.25 nm). We first assume that the intrinsic quantum yield is 100% then we will modify that assumption. [Pg.300]

It is important to point out here, in an early chapter, that the Born-Oppenheimer approximation leads to several of the major applications of isotope effect theory. For example the measurement of isotope effects on vapor pressures of isotopomers leads to an understanding of the differences in the isotope independent force fields of liquids (or solids) and the corresponding vapor molecules with which they are in equilibrium through use of statistical mechanical theories which involve vibrational motions on isotope independent potential functions. Similarly, when one goes on to the consideration of isotope effects on rate constants, one can obtain information about the isotope independent force constants which characterize the transition state, and how they compare with those of the reactants. [Pg.60]

Extraction process, 26 381 Extractive chemisorption, 37 80 Extra-framework titanium, 41 293 Extrinsic field effect, 27 26-48 catalysts for, 27 49 theory, 27 50, 51 Extrusion, 28 83... [Pg.104]

Topsom, 1976) and to treat them separately. In this review we will be concerned solely with polar or electronic substituent effects. Although it is possible to define a number of different electronic effects (field effects, CT-inductive effects, jt-inductive effects, Jt-field effects, resonance effects), it is customary to use a dual substituent parameter scale, in which one parameter describes the polarity of a substituent and the other the charge transfer (resonance) (Topsom, 1976). In terms of molecular orbital theory, particularly in the form of perturbation theory, this corresponds to a separate evaluation of charge (inductive) and overlap (resonance) effects. This is reflected in the Klopman-Salem theory (Devaquet and Salem, 1969 Klop-man, 1968 Salem, 1968) and in our theory (Sustmann and Binsch, 1971, 1972 Sustmann and Vahrenholt, 1973). A related treatment of substituent effects has been proposed by Godfrey (Duerden and Godfrey, 1980). [Pg.132]

Fibrillin, calcium binding, 46 473, 474, 477 Fibulin-I, calcium binding, 46 473 Field desorption mass spectroscopy, 28 6, 21 Field effects, of astatophenols, 31 66 Fine structure, 13 193-204 Fingerprinting of polymetalates, 19 246-248 Finite perturbation theory, 22 211, 212 First transition series, substitution, transferrins, 41 423 26... [Pg.105]

Fig. 20 Charge carrier mobility in P3HT as a function of the charge carrier concentration. Squares refer to an experiment performed on a field effect transistor while circles refer to experiments done on an electrochemically doped sample. In the latter case the mobility is inferred from the steady state current at a given doping level. Solid and dashed lines have been fitted using the theory of [101]. The fit parameters are the site separation a, the prefactor Vq in the Miller-Abrahams-type hopping rate, the inverse wavefunction decay parameter y and the dielectric constant e. From [101] with permission. Copyright (2005) by the American Institute of Physics... Fig. 20 Charge carrier mobility in P3HT as a function of the charge carrier concentration. Squares refer to an experiment performed on a field effect transistor while circles refer to experiments done on an electrochemically doped sample. In the latter case the mobility is inferred from the steady state current at a given doping level. Solid and dashed lines have been fitted using the theory of [101]. The fit parameters are the site separation a, the prefactor Vq in the Miller-Abrahams-type hopping rate, the inverse wavefunction decay parameter y and the dielectric constant e. From [101] with permission. Copyright (2005) by the American Institute of Physics...
Calculations of the external electric field effect on the escape probability in multipair clusters [18] have shown that significant deviations from the results of the single-pair theory are expected at high electric fields. At low fields, the escape probability is a linear... [Pg.268]

Computer simulation has also been used to calculate the external electric field effect on the geminate recombination in high-mobility systems [22]. For the mean free time x exceeding -0.05, the field dependence of the escape probability was found to significantly deviate from that obtained from the diffusion theory. Furthermore, the slope-to-intercept ratio of the field dependence of the escape probability was found to decrease with increasing x. Unlike in the diffusion-controlled geminate recombination, this ratio is no longer independent of the initial electron-ion separation [cf. Eq. (24)]. [Pg.271]

A thorough discussion Is given of the field modulation technique, a new stationary relaxation method based on electric field perturbation of Ionic equilibria. Concomitantly the theory of electric field effect In Ionic systems Is reviewed especially stressing their Importance for conductance phenomena In low polar solutions. [Pg.153]

Satyavratam and Vedam also make the important point that the theory of underwater energy measurements was developed for relatively far-field effects, whereas the performance of commercial... [Pg.93]


See other pages where Field Effect Theory is mentioned: [Pg.23]    [Pg.50]    [Pg.23]    [Pg.50]    [Pg.381]    [Pg.175]    [Pg.170]    [Pg.323]    [Pg.227]    [Pg.48]    [Pg.288]    [Pg.290]    [Pg.610]    [Pg.283]    [Pg.96]    [Pg.294]    [Pg.124]    [Pg.150]    [Pg.178]    [Pg.178]    [Pg.128]    [Pg.472]    [Pg.56]    [Pg.147]    [Pg.32]    [Pg.276]    [Pg.318]    [Pg.132]    [Pg.677]    [Pg.657]    [Pg.78]    [Pg.431]   


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Effective magnetic field parameter theory

Extrinsic field effect theory

Landau theory magnetic field effects

Magnetic field effects theory

Symmetry energy effective field theory

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