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Dipolar response

Here the ijk coordinate system represents the laboratory reference frame the primed coordinate system i j k corresponds to coordinates in the molecular system. The quantities Tj, are the matrices describing the coordinate transfomiation between the molecular and laboratory systems. In this relationship, we have neglected local-field effects and expressed the in a fomi equivalent to simnning the molecular response over all the molecules in a unit surface area (with surface density N. (For simplicity, we have omitted any contribution to not attributable to the dipolar response of the molecules. In many cases, however, it is important to measure and account for the background nonlinear response not arising from the dipolar contributions from the molecules of interest.) In equation B 1.5.44, we allow for a distribution of molecular orientations and have denoted by () the corresponding ensemble average ... [Pg.1290]

Alderscv Willi.jniv H. The Most Beautiful Molecule The Discovery of the Buclty-halL John Wiley Sons. Inc.. New York. NY. 1997 Aleis. G.B.. et at. "E-vislence of an Orientational Electric Dipolar Response in ( hi Single Cryslals." Science. 511 iJllll 24. 1992). [Pg.288]

On the other hand DRS is complex and fraught with potential problems, for example, under the effect of the applied field, there is ionic migration and the ionic conductivity term must be deconvolved from the dipolar response at lower frequencies. Moreover DRS is technologically demanding and expensive and only well trained personnel can exploit its potential [99,100]. [Pg.21]

Figure 3.1 Cartoon for an excited PTCDA molecule and the silver island dipolar response that results in significant radiation. Figure 3.1 Cartoon for an excited PTCDA molecule and the silver island dipolar response that results in significant radiation.
The dipolar response of a large sodium sphere can be calculated from the experimental bulk dielectric function as discussed in the context of Eq. (6). The calculated width is To = 0.19 eV. This asymptotic experimental width is due to a structure in the dielectric function which is caused by an interband transition [55]. The collective oscillation can decay by exciting a single electron to a higher electronic band. The same mechanism occurs in the damping of the bulk plasmon. In this case, the width can be well correlated with the strength of the pseudopotential (see Figure 9 of Ref. [48]). [Pg.203]

In formulating the general theory it is helpful first to establish the dipolar response of each ion, atom, chromophore or molecule to the oscillating electric field of the radiation. This is associated with an interaction operator ... [Pg.1154]

There are higher multipole polarizabilities tiiat describe higher-order multipole moments induced by non-imifonn fields. For example, the quadnipole polarizability is a fourth-rank tensor C that characterizes the lowest-order quadnipole moment induced by an applied field gradient. There are also mixed polarizabilities such as the third-rank dipole-quadnipole polarizability tensor A that describes the lowest-order response of the dipole moment to a field gradient and of the quadnipole moment to a dipolar field. All polarizabilities of order higher tlian dipole depend on the choice of origin. Experimental values are basically restricted to the dipole polarizability and hyperpolarizability [21, 24 and 21]. Ab initio calculations are an imponant source of both dipole and higher polarizabilities [20] some recent examples include [26, 22] ... [Pg.189]

NITRILE OXIDES. Nitrile oxides are a well known class of compds represented by R.C N- 0, and are usually prepd by treating hydroxamic acid chlorides with a mild alkali, thus eliminating HQ (Ref 2). Wieland (Refs 1 3) was responsible for the first isolation of free nitrile oxides. These compds are somewhat unstable, showing a marked tendency to dimerize to (he corresponding furoxanes (1,3-dipolar addition) (Refs 2 3). The nitrile oxides add to a considerable number of carbenes, as benzonitrUe oxide (for example) to a large number of olefins in ether at 20° (Ref 3)... [Pg.288]

The model in Figure 3.20a applies to ACM-silica, while Figure 3.20b suits the ENR-silica system. Kraus constant, C, determined from the slope of the plots in Figure 3.19, quantifies the mbber-silica interaction in these systems. CACM/siUca is 1-85 and CENR/siika is 2.30 and these values are significantly higher than the reinforcing black-filled mbber composites [65]. Hydrogen-bonded interaction between the SiOH and the vicinal diols in ENR is responsible for this, whereas dipolar interaction between ester and SiOH in ACM-silica only results in weaker adsorption of the mbber over the filler surfaces. [Pg.76]

Dipolar coupling The direct through-space coupling interaction between two nuclei. It is responsible for nOe and relaxation, and represents the... [Pg.413]

The energy available from the anthracene triplet (42 kcal/mole) is sufficient to produce either of these states. The singlet excited molecule subsequently attacks a ground state anthracene to produce the observed endoperoxide. The 1Aff state is believed to be responsible for the addition to anthracene to form the endoperoxide since it closely resembles a diradical species, while the 1Ss+ state more closely resembles a dipolar ion. [Pg.342]


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