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Hyperpolarizability tensor

B1.3.2.5 THE MICROSCOPIC HYPERPOLARIZABILITY TENSOR, ORIENTATIONAL AVERAGING, THE KRAMERS-HEISENBERG EXPRESSION AND DEPOLARIZATION RATIOS... [Pg.1189]

The other major properties computed by a frequency job are the polarizability and hyperpolarizability tensors. Normally, the polarizability is printed at the end of the output, just before the archive entry ... [Pg.69]

In a normal Hartree-Fock job, the hyperpolarizability tensor is given only in the archive entry, in the section beginning HyperPolar=. This tensor is also in lower tetrahedral order, but expressed in the input (Z-matrix) orientation. (This is also true of the polarizability tensor within the archive entry.)... [Pg.69]

If you begin the route section with P rather than T, then additional information is printed at various points in the job. One of these items is a display of the polarizability and hyperpolarizability tensors much earlier in the output, just prior to the frequency results ... [Pg.70]

Coupled Hartree-Fock Approach to Electric Hyperpolarizability Tensors in Benzene... [Pg.279]

Table 1 Theoretical electric hyperpolarizability tensor of benzene molecule (in a.u.). ... Table 1 Theoretical electric hyperpolarizability tensor of benzene molecule (in a.u.). ...
Trans-polyenes H-(-HC=CH-),, -H, trans-polyenynes H-(HC=CH-C=C) -H, cumulenes H2C=(C=C) =CH2 and polyynes H-(C=C) -H have been studied (M=N-1). For eentrosymmetrie molecules, the first order hyperpolarizability p is equal to zero so that non linear effects are of second order nature. Furthermore, (the x axis goes through the middle of the C-C bonds of the polyenes, or is the intemuclear axis in the case of linear molecules) is the most important component of the second order y hyperpolarizability tensor, the other components being negligible. Both y and the mean hyperpolarizability... [Pg.297]

Coupled Hartree-Fock approach to electric hyperpolarizability tensors in benzene... [Pg.472]

Before closing this section, it is worth mentioning that the hyperpolarizability tensors are complex quantities usually given in the old cgs system of units of esu (electrostatic units). The transformation into the International System is readily obtained with the relationship ... [Pg.143]

The SH signal directly scales as the square of the surface concentration of the optically active compounds, as deduced from Eqs. (3), (4), and (9). Hence, the SHG technique can be used as a determination of the surface coverage. Unfortunately, it is very difficult to obtain an absolute calibration of the SH intensity and therefore to determine the absolute number for the surface density of molecules at the interface. This determination also entails the separate measurement of the hyperpolarizability tensor jS,-, another difficult task because of local fields effects as the coverage increases [53]. However, with a proper normalization of the SH intensity with the one obtained at full monolayer coverage, the adsorption isotherm can still be extracted through the square root of the SH intensity. Such a procedure has been followed at the polarized water-DCE interface, for example, see Fig. 3 in the case of 2-( -octadecylamino)-naphthalene-6-sulfonate (ONS) [54]. The surface coverage 6 takes the form ... [Pg.144]

The hyperpolarizability tensor is obtained in a way similar to the case of SHG. However, the selection rules for an SFG resonance at the IR frequency implies that the vibrational mode is both IR and Raman active, as the SF hyperpolarizability tensor elements involve both an IR absorption and a Raman-anti-Stokes cross-section. Conversely, the DFG hyperpolarizability tensor elements involve an IR absorption and a Raman-Stokes cross-section. The hyperpolarizability tensor elements can be written in a rather compact form involving several vibrational excitations as [117] ... [Pg.157]

Heterogeneous dielectric media models have included the developments of Jprgensen et al. [7-9] (reviewed here) and Corni and Tomasi [52,53], Generally, the number of methods for determining frequency-dependent molecular electronic properties, such as the polarizability or first- and second hyperpolarizability tensors of heterogeneously solvated molecules, is very limited. [Pg.282]

Our present focus is on correlated electronic structure methods for describing molecular systems interacting with a structured environment where the electronic wavefunction for the molecule is given by a multiconfigurational self-consistent field wavefunction. Using the MCSCF structured environment response method it is possible to determine molecular properties such as (i) frequency-dependent polarizabilities, (ii) excitation and deexcitation energies, (iii) transition moments, (iv) two-photon matrix elements, (v) frequency-dependent first hyperpolarizability tensors, (vi) frequency-dependent polarizabilities of excited states, (vii) frequency-dependent second hyperpolarizabilities (y), (viii) three-photon absorptions, and (ix) two-photon absorption between excited states. [Pg.538]

Based on the MCSCF/CM quadratic response method it is possible to calculate the hyperpolarizability tensor and the two-photon absorption cross-sections. The calculated MCSCF/CM properties exhibit for all the individual tensor components substantial shifts compared with the corresponding molecular properties of the molecule in vacuum. [Pg.554]

For dipolar chromophores that are the subject of this chapter, only one component of the molecular hyperpolarizability tensor, Pzzz, is important. Thus, the summation in Eq. (8) disappears. Electric field poling induces Cv cylindrical polar symmetry. Assuming Kleinman [12] symmetry, only two independent components of the macroscopic second-order nonlinear optical susceptibility tensor... [Pg.10]

The conjugated molecules are elongated with a much better electron mobility in the backbone direction than perpendicular to it. The dipole and transition dipole moments are pointing in this direction (x) with Consequently, the second-order hyperpolarizability tensor y is dominated by... [Pg.161]

For the two-dimensional (2D) conjugated molecules the second-order hyperpolarizability tensor elements Yijki with an index in z direction (perpendicular to the conjugation plane) can be neglected with the same arguments as for the ID molecules. [Pg.162]


See other pages where Hyperpolarizability tensor is mentioned: [Pg.1189]    [Pg.1195]    [Pg.223]    [Pg.284]    [Pg.141]    [Pg.147]    [Pg.148]    [Pg.149]    [Pg.157]    [Pg.194]    [Pg.194]    [Pg.27]    [Pg.530]    [Pg.262]    [Pg.264]    [Pg.354]    [Pg.164]    [Pg.169]    [Pg.195]    [Pg.352]    [Pg.472]    [Pg.658]    [Pg.178]    [Pg.178]    [Pg.388]    [Pg.177]    [Pg.282]    [Pg.302]    [Pg.64]   
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See also in sourсe #XX -- [ Pg.554 ]

See also in sourсe #XX -- [ Pg.304 , Pg.305 ]

See also in sourсe #XX -- [ Pg.206 ]

See also in sourсe #XX -- [ Pg.144 ]

See also in sourсe #XX -- [ Pg.369 ]




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Electric hyperpolarizability tensor, quadratic

Frequency-dependent first hyperpolarizability tensors

Hyperpolarizabilities

Hyperpolarizability

Hyperpolarizability tensor factors

Hyperpolarizability tensor media

Hyperpolarizability tensor perturbation

Hyperpolarizability tensor single molecule

Hyperpolarizability tensors, first

Hyperpolarizability tensors, molecular

Hyperpolarizability tensors, nonlinear optical

Molecular first hyperpolarizability tensor

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