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Dielectric response function

In its underlying physics, the use of susceptibilities to obtain E is related to the use of a generalized dielectric response function to determine the energy of a... [Pg.172]

The wave vector, k , and the screening length, 1/ , depend only on the density of the free-electron gas through the poles of the approximated inverse dielectric response function, whereas the amplitude, A , and the phase shift, a , depend also on the nature of the ion-core pseudopotential through eqs (6.96) and (6.97). For the particular case of the Ashcroft empty-core pseudopotential, where tfj fa) = cos qRc, the modulus and phase are given explicitly by... [Pg.158]

The effects of coupling of the DTO and RB units in not only one- but also three-dimensional arrays are discussed below and molecular weight trends illustrated. A fundamental connection between relaxation times and normal mode frequencies, shown to hold in all dimensions, allows the rapid derivation of the common viscoelastic and dielectric response functions from a knowledge of the appropriate lattice vibration spectra. It is found that the time and frequency dispersion behavior is much sharper when the oscillator elements are established in three-dimensional quasi-lattices as in the case of organic glasses. [Pg.104]

As a result of these very general considerations, one expects the dielectric response function, as expressed by the complex permittivity, k (oj), or the attenuation function, a(oi), of ordinary molecular fluids to be characterized, from zero frequency to the extreme far-infrared region, by a relaxation spectrum. To first order, k (co) may be represented by a sum of terms for individual relaxation processes k, each given by a term of the form ... [Pg.3]

Equation 1.79 is the basis for a measurement method of the dielectric response function /ft). Upon connecting the switch of the circuit shown in Figure 1.28, a polarization current, ipolft), through the capacitor can be recorded, according to the following equation... [Pg.44]

The methodology for the calculation of the complex relative permittivity for the dipolar relaxation mechanism is founded on the calculation of the dielectric response function, f(t), for a depolarization produced by the discharge of a previously charged capacitor. In Figure 1.29a, a circuit is shown where a capacitor is inserted in which a dipolar dielectric material is enclosed in the parallel plate capacitor of area, A, and thickness, d, with empty capacitance C0 = Q0/U0 = 0(A/d), and E0 = U0ld. In Figure 1.29b, the corresponding depolarization process is shown. [Pg.45]

At visible frequencies, the change in the solution index of refraction with an added solute gives a qualitative idea of the magnitude of relative polarizability of solute and solvent. As elaborated elsewhere in the text, the complex dielectric response, e = e (a>) + is"(co), is equal to the square of the complex refractive index ( ref + /kabs)2 = (w2ef— Kbs) + 2i reffcabs where nKi is the index of refraction and kabs is the absorption coefficient. In a transparent region where kabs = 0, the dielectric response function e = njref. (See the Level 2.4 essay on dielectric response.)... [Pg.83]

The opening Notation section, Section L2.1, applies not only to the tables but also to the texts of Levels 1 and 2. The Essays on formulae section, Section L2.3, which immediately follows the tables sections, reduces the results from Level 3 derivations to simpler forms. The Computation section, Section L2.4, sketches the physical foundations of the all-important dielectric-response functions and gives mathematical guidelines for calculation. [Pg.100]

Let region m be a pure salt solution with dielectric-response functions em and with a valence-weighted sum of concentrations (as number densities)... [Pg.224]

It is not necessary to consider spheres only. For any particular system the dielectric-response functions and excess ion densities can be measured or formulated as functions of the size, shape, and charge of the suspended particles as well as from ionic properties of the bathing solution. It is a separate procedure to compute the excess numbers Tv from mean-field theory. They are used here as given quantities. [Pg.225]

There are also a number of theories taking into account dipolar solvation dynamics. These theories use the solvent s dielectric response function as the dynamical input and also include effects due to the molecular nature of the solvent. The most sophisticated of these theories, by Raineri et al. [136] and by Friedman [137], uses fully atomistic representations for both solute and solvent and recent comparisons have shown it to be capable of quantitatively reproducing both the static and dynamic aspects of solvation of C153 [110]. In these cases the theoretical nature of solvation dynamics is fully understood. However, it must be remembered that much of the success of these theories rests on using the dynamical content of the complicated function, dielectric response function, determined from experiment. Although there... [Pg.314]

Finally, it should be noted that IL-CT mixing in the lowest triplet for any given [Re(L)(CO)3(N,N)] is strongly medium dependent. 3CT state energies are much more sensitive to medium variations than 3IL. Essentially, any change in the medium (liquid-to-solid transition, decrease in the dielectric response function,... [Pg.93]

Although many improvements have been proposed for the calculation of the dielectric response function from first principles [31,32], still this stage is both computer time and memory very demanding when a large basis set is used for the description of the electronic structure. Efficient GW methods have thus been developed, in which a model dielectric function is used to mimick the screening properties of the system under study [28,33,34]. [Pg.42]

To end up this Section, we consider now an alternative ASC approach which strongly deviates from the basic set up previously discussed. The quantum system, the solute , has been considered immersed in a continuum solvent distribution characterized, pritna facie, by its dielectric response function. Klamt and Schuiirman (1993) propose to replace the dielectric response function with the response function of a liquid electric conductor (the so-called COSMO model). In doing so, one has other electrostatic problems, with simpler boundary conditions. In fact, for a system of charges (the solute) in a screening conductor (where = oo), the electro-... [Pg.57]

In order to calculate dielectric response functions, we suppose that a uniform field F (having been applied to the assembly of dipoles at a time t = — oo so that equilibrium conditions prevail by the time t 0) is switched off at t = 0. In addition, we suppose that the field is weak (i.e., pF linear response condition [8]). Thus the initial distribution function W(<)>, 0) is the Boltzmann distribution function and is given by Eq. (57). Now one can readily obtain the corresponding aftereffect solution... [Pg.320]

As indicated above, exponential relaxation does not generally provide a satisfactory description of experimental data. The response of dielectric materials is instead generally found to be characterized by certain power laws, both in the time and frequency domains (95,96). As observed by Curie and von Schweidler, a long time ago (97,98), the polarization current following the application of a constant electric field typically decays as a power function of time. The same is true for the dielectric response function, since it is proportional to the current oc l/t , where a is a positive constant. This response... [Pg.443]

We consider a polar solvent characterized by its dielectric response function s co). Upon a sudden change in the charge distribution inside this solvent a relaxation process follows in which the solvent adjusts to the new charge distribution. We want to describe this relaxation process in terms of the (assumed known) dielectric response function. ... [Pg.539]

Following Marcus, we simplify this picture by assuming that the solvent is characterized by only two timescales, fast and slow, associated, respectively with its electronic and the nuclear response. Correspondingly, the solvent dielectric response function is represented by the total, or static, dielectric coefficient Sg and by its fast electronic component Sg (sometimes called optical response and related to the refraction index n by Sg = n ). includes, in addition to the fast electronic component, also contributions from solvent motions on slower nuclear timescales Translational, rotational, and vibrational motions. The working assumption of the... [Pg.559]

Thus, Eqs (18.98)—(18.109) provide a microscopic expression for the dielectric response function in a system of noninteracting particles... [Pg.701]

Having obtained expressions for the dielectric susceptibility and the dielectric response functions in terms of microscopic variables, we may proceed to express other observables in microscopic terms. Consider an electromagnetic mode whose electric component is described by a plane wave propagating in the x direction in an isotropic medium, and assume that the field is weak enough to make linear response theory valid. The field is given by... [Pg.701]

S (q, to) is connected to the polarizability x(q, ro) in the way shown in Equation (3). Let us turn to the most simple model case, the jellium model, in which the electrons are assumed to be free particles, moving embedded in a positive uniform charge background, obeying only Pauli s principle but not showing any electron-electron interactions. For this case of a non-interacting electron gas, the dielectric response function is given by... [Pg.180]

Two points should be mentioned here. First, the effect of solutes on the solvent dielectric response can be important in solvents with nonlocal dielectric properties. In principle, this problem can be handled by measuring the spectrum of the whole system, the solvent plus the solutes. Theoretically, the spatial dependence of the dielectric response function, s(r, co), which includes the molecular nature of the solvent, is often treated by using the dynamical mean spherical approximation [28, 36a, 147a, 193-195]. A more advanced approach is based on a molecular hydrodynamic theory [104,191, 196, 197]. These theoretical developments have provided much physical insight into solvation dynamics. However, reasonable agreement between the experimentally measured Stokes shift and emission line shape can be... [Pg.520]


See other pages where Dielectric response function is mentioned: [Pg.191]    [Pg.191]    [Pg.34]    [Pg.366]    [Pg.77]    [Pg.196]    [Pg.104]    [Pg.291]    [Pg.9]    [Pg.17]    [Pg.43]    [Pg.47]    [Pg.50]    [Pg.262]    [Pg.315]    [Pg.7]    [Pg.21]    [Pg.395]    [Pg.375]    [Pg.376]    [Pg.377]    [Pg.180]   
See also in sourсe #XX -- [ Pg.77 ]

See also in sourсe #XX -- [ Pg.152 ]

See also in sourсe #XX -- [ Pg.22 ]




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