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Biorthogonal functions

Extending the structure of the wave function is not the only way of improving the APSG approximation. In our laboratory [109, 107, 108], we proposed the biorthogonal formulation to take care of intergeminal overlap effects, and derived simple formulae to account for delocalization and dispersion interactions using either perturbation theory or a linearized coupled-cluster-type ansatz with the APSG reference state. [Pg.70]

We now restrict ourselves to periodic functions V x) of x, so that we may impose periodic boundary conditions. Thus directly proportional to the equilibrium distribution. The probability density P may now be written in terms of the so-called biorthogonal expansion given by Morse and Feschbach [61]... [Pg.423]

Fig. 14 An example of biorthogonal scaling and wavelet functions with their duals. Fig. 14 An example of biorthogonal scaling and wavelet functions with their duals.
A biorthogonal scaling and wavelet function are semiorthogonal if they generate an orthogonal multiresolution analysis... [Pg.83]

Chau and his co-workers have proposed some wavelet-based methods to compress UV-VIS spectra [24,37]. In their work, a UV-VIS spectrum was processed with the Daubechies wavelet function, Djfi. Then, all the Cj elements and selected Dj coefficients at different) resolution levels were stored as the compressed spectral data. A hard-thresholding method was adopted for the selection of coefficients from Dj. A compression ratio up to 83% was achieved. As mentioned in the previous section, the choice of mother wavelets is vast in WT, so one can select the best wavelet function for different applications. Flowever, most workers restrict their choices to the orthogonal wavelet bases such as Daubechies wavelet. Chau et al. chose the biorthogonal wavelet for UV VIS spectral data compression in another study [37]. Unlike the orthogonal case, which needs only one mother wavelet (p(t), the biorthogonal one requires two mother wavelets. (p(t) and (p(t), which satisfy the following biorthogonal property [38] ... [Pg.252]

As discussed earlier, the present interpretation of the truth table can be obtained from conventional representations with the use of a non-positive definite metric A All = —A22=1 Ai2=Ai2=0. In this picture, we can use conventional brake nomenclature, while for another selection of A, leading e.g. to a complex symmetric choice, it would require complex symmetric realisations. In both cases, the formulation is biorthogonal. With this realisation, we can make an identification between Eqs. (1.63) and (1.66), making the replacement q = /c(r), where q is related to the probability function/operator of the simple proposition Q = P. Hence, we realise a probabilistic origin combined with the nonclassical, self-referential character of gravitational interactions. Note also the analogy between the formulations, i.e. that the result of a classical measurement, i.e. the truth or... [Pg.20]

In this paper we use biorthogonal wavelets on the interval constructed by (Cema Finek 2008 Cerna Finek 2009) which outperforms similar construction in the sense of better conditioning of base functions as well as in better conditioning of wavelet transform. The condition number seems to be nearly optimal most especially in the case of cubic spline wavelets. From the viewpoint of numerical stabihty, ideal wavelet bases are orthogonal wavelet bases. However, they are... [Pg.820]

Owing to the presence of the antihermitian part of the eigenfunctions n> are not orthogonal, and they must be combined with conjugate functions [Pg.326]

Bloch function (p. 435) symmetry orbital (p. 435) biorthogonal basis (p. 436) inverse lattice (p. 436)... [Pg.495]

We note that the incoming wave boundary conditions in the bra state in Eqs. (2.2) and (2.4) can be enforced by not complex conjugating radial functions in bra states of Eq. (2.7). This inner product is called the biorthogonal inner product [29], and is formally related to the use of complex scaled coordinates and absorbing boundary conditions. [Pg.22]

However, since the bra states are used only for projection of the coupled-cluster equations (which is zero for the optimized wave function), normalization is unimportant. In fact, use of the biorthogonal basis (13.7.59) rather than the biorthonormal basis (13.7.60) simplifies our algebraic manipulations considerably. [Pg.170]


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See also in sourсe #XX -- [ Pg.108 , Pg.135 , Pg.150 ]




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Biorthogonality

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