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Vibrational contribution and

As mentioned in the previous section, the temperature-dependent absorption spectra of RCs are very important for the understanding of the molecular properties such as the electronic configurations, vibrational contributions, and transition moment relations of the Bchls in RCs. However, only in the R26. Phe-a mutant case have absorption spectra at various temperatures so far been available. Although the absorption spectra of the WT and R26 mutant RCs are available at a few temperatures like IK, 4K, 77K, and 298K, the analyzed results are not so consistent (see Table III). It may be because the preparation... [Pg.23]

Figure 19. Comparison of calculated and measured signals using the M(t) shown in Fig. 18. (a) Three-pulse echo peak shift, (b) transient grating, and (c) transient absorption. A pulse duration of 16 fs (20 fs for transient grating) and a detuning of 230 cm-1 are used in the calculated signals. The peak near T = 0 in the transient grating and transient absorption signals, usually referted to as the coherent artifact, arises from the ultrafast decay (sum of intramolecular vibrational contribution and -100 fs ultrafast solvation dynamics) in M(t). Figure 19. Comparison of calculated and measured signals using the M(t) shown in Fig. 18. (a) Three-pulse echo peak shift, (b) transient grating, and (c) transient absorption. A pulse duration of 16 fs (20 fs for transient grating) and a detuning of 230 cm-1 are used in the calculated signals. The peak near T = 0 in the transient grating and transient absorption signals, usually referted to as the coherent artifact, arises from the ultrafast decay (sum of intramolecular vibrational contribution and -100 fs ultrafast solvation dynamics) in M(t).
The calculations give the electronic part of the polarizability. It is thought that the ZPYA correction is the major part of the vibrational contribution and has a value of about 0.29 au at zero frequency. In Table 6 this correction has been added to the electronic part to give the values in the final column, which can be compared with the two possible experimental values in the first two rows. The most accurate of the CCSD type work should be that of Christiansen... [Pg.78]

The purpose of this chapter is to introduce the fundamentals of the theory of linear and nonlinear optical processes, and our focus will be on the general features of the theory. We will primarily restrict our discussion to the framework of exact-state Aieories, and focus on the occurrence of linear and nonlinear optical processes from a physical point of view. However, in order to set a frame of reference we provide a brief outline of the most common classes of meAiods in approximate-state theories. We will discuss the partitioning of molecular properties into electronic and vibrational contributions, and close the chapter wlAi a brief discussion of the comparison of Are microscopic properties with those of the bulk. We wish to stress that other chapters of this book will cover these latter aspects in greater detail. [Pg.2]

The main conclusion is that the success of this field is due to a close interconnection between analytical and computational approaches. The paper has clearly demonstrated that we need to take into account electron-phonon interactions. In other terms, there exists a timely need to include translational, rotational, vibrational contributions and non-adiabatic approaches in our models. Then the road will be open to complete non-equilibrium interpretations of the electronic properties of macromolecules [89]. [Pg.1041]

Polarizabilities a (without the vibrational contribution) and the components a, (parallel) and (perpendicular to the molecular symmetry axis) from three theoretical calculations are given below ... [Pg.156]

Table 4 shows experimental and calculated first dissociation energies at different levels of theory for the homoleptic TM carbonyls M(CO) . Table 5 shows theoretical and experimental M-L bond dissociation energies for substituted carbonyls M(CO)5L. Since zero-point vibrational contributions and thermal contributions at room temperature to the dissociation energy nearly cancel each other, it is justified to compare energy differences D with experimental dissociation energies Do The following conclusions can be drawn from the theoretical dissociation energies obtained at different levels of theory ... [Pg.3077]

In Table 15.29, we have listed the reaction enthalpies of the 17 isogyric reactions examined in the present section. At T = OK, the total enthalpy of a reaction may be decomposed into a nonrelativistic electronic equilibrium contribution, a vibrational contribution and a relativistic correction ... [Pg.343]


See other pages where Vibrational contribution and is mentioned: [Pg.275]    [Pg.155]    [Pg.155]    [Pg.66]    [Pg.67]    [Pg.28]    [Pg.370]    [Pg.16]    [Pg.235]    [Pg.493]    [Pg.45]    [Pg.82]    [Pg.89]    [Pg.3]    [Pg.127]    [Pg.135]    [Pg.385]    [Pg.319]    [Pg.309]    [Pg.56]    [Pg.39]    [Pg.16]   
See also in sourсe #XX -- [ Pg.392 , Pg.393 ]




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Vibrational contributions

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