Distortion, diagonal

Here the distortion (diagonal) and back coupling matrix elements in the two-level equations (section B2.2.8.4) are ignored so that = exp(ik.-R) remains an imdistorted plane wave. The asymptotic solution for ij-when compared with the asymptotic boundary condition then provides the Bom elastic ( =f) or inelastic scattering amplitudes... 

In conclusion we propose ASR as an efficient computational scheme to study electronic structure of random alloys which allows us to take into account the coherent scattering from more than one site. Consequently ASR can treat effects such as SRO and essential off-diagonal disorder due to lattice distortion arising out of size mismatch of the constituents. 

Figure 23. This caricature demonstrates the predicted phenomena of energy level crossing in domains whose energy bias is comparable or larger than the vibronic frequency of the domain wall distortions. The vertical axis is the energy measured from the bottom state the horizontal axis denotes temperature. The diagonal da ed line denotes roughly the thermal energies. A tunneling center that would become thermally active at some temperature Tq will not possess ripplons whose frequency is less than To.

The distance between the diagonal nitrogen atoms is approximately 4 A [ 12]. The distortion induced by the incorporated metal is negUgible and planar four-coordinated metallocomplexes are produced. Therefore, the metal-nitrogen dis-... 

We introduced the technique for measuring the weak interaction forces acting between two particles using the photon force measurement method. Compared with the previous typically used methods, such as cross-correlation analysis, this technique makes it possible to evaluate the interaction forces without a priori information, such as media viscosity, particle mass and size. In this chapter, we focused especially on the hydrodynamic force as the interaction between particles and measured the interaction force by the potential analysis method when changing the distance between particles. As a result, when the particles were dose to each other, the two-dimensional plots of the kinetic potentials for each particle were distorted in the diagonal direction due to the increase in the interaction force. From the results, we evaluated the interaction coeffidents and confirmed that the dependence of the... 

Unlike Eqs. (8), the first of Eqs. (13) involves only part of the interaction of the electron with the medium polarization V P, which, together with VeA, creates the potential well for the electron near the donor A. As for the interaction with the polarization V%, which, together with VeB, creates the potential well for the electron near the acceptor, the first of Eqs. (13) involves only the diagonal part of this interaction, VfP, leading to a distortion of the state A without a change in the electron localization. The state B is determined in a similar way. 

Because we are concerned only with the analysis of the absorption spectra of P band and B band, we consider the excitonic interactions among P, BL, and BM shown in Fig. 8. Here (oti, ot2,0C3,014) represent the diagonal matrix elements, while (p, (314, P23, P34) represent the off-diagonal matrix elements [67]. As shown in Introduction, a main feature of the P band is that its absorption maximum shows a pronounced temperature shift [42,52], According to the displaced oscillator model, the absorption maximum is independent of T. Although the distortion effect of potential surfaces will introduce some temperature shift, the effect cannot be as large as that shown in Fig. 2. 

Wade expanded the 1971 hypothesis to incorporate metal hydrocarbon 7T complexes, electron-rich aromatic ring systems, and aspects of transition metal cluster compounds [a parallel that had previously been noted by Corbett 19) for cationic bismuth clusters]. Rudolph and Pretzer chose to emphasize the redox nature of the closo, nido, and arachno interconversions within a given size framework, and based the attendant opening of the deltahedron after reduction (diagonally downward from left to right in Fig. 1) on first- and second-order Jahn-Teller distortions 115, 123). Rudolph and Pretzer have also successfully utilized the author s approach to predict the most stable configuration of SB9H9 (1-25) 115) and other thiaboranes. 

If cross peaks are of unequal volumes, aij Tm) a,ji Tm), owing to short repetition time or spectral distortions, it is best to normalize the geometric mean of the cross peaks by the geometric mean of their respective diagonals. Although approximate, eq. (30) is useful because errors of peak volumes often exceed errors introduced by the truncated Taylor expansion. The limitations and criteria for the validity of Taylor expansion are described elsewhere [55]. 

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