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Integrals asymptotic forms

L sirif Lhc above asymptotic forms of the two-ceiiLer Lwo-dccLron integrals, the paramelers A. and can he derived. C. ertainly, parameter A. is different for different orbitals even though they reside on the same atom, Dewar used AM to represent the parameter A obtained via AD to represent the parameter A obtained via and AQ to represent the parameter A obtained from Hpp-... [Pg.289]

A sequence of approximations, using properties of the confluent hypergeometric function, integration by steepest descents, and judicious discard of all but the dominant terms, gives one the asymptotic form... [Pg.255]

In the preceding paragraphs of this section we have summed the terms arising from the partial expansion of the exponentials occurring in the coefficients of the powers of particle concentrations to obtain a series of multiple infinite sums, the terms of which are convergent. The terms in S(R) are of the same form as those in the Mayer solution theory, apart from replacement of integration by summation and the fact that mu differs from the solution value because of the discreteness of the lattice. The evaluation of wi - is outlined in the next section. It is found that the asymptotic form is... [Pg.56]

Fig. 6.23 a Comparison of the universal Zimm relaxation function F(x) to stretched exponentials. The dotted line is the residual error xlO to the best fit (a=1.354, =0.852). The p value of 2/3 only applies at large values of x with F(x)< 10 , which are irrelevant for NSE data. The dashed blue line in the right part of the figure corresponds to the asymptotic form given in [6] exp(-1.35x ). b Comparison of the integration result solid line), the approximation Eq. 6.48 dashed line) and the asymptotic form dashed-dotted line). Only for very large values of x>30 does the asymptotic value of p emerge... [Pg.194]

The long-range asymptotic form of the exchange potential, a constituent of the exchange-correlation potential (56), will be discussed in this and the remaining subsections. Since the known derivations of this form are very complicated and involve an analysis of an integral equation of the OP method (see, e.g. [17], [27],... [Pg.78]

The line-integral approximation [ ]), Eq. (213) with (211) or (216), to the exact u,(r [n]) seems to be especially accurate. First of all, its asymptotic behavior for pure-state systems is the same as the behavior of the exact r, in Eq. (134), therefore guaranteeing the proper asymptotic form of KS orbitals. Next, it satisfies exactly the Levy-Perdew [33] identity... [Pg.93]

Since the only contributions to eq. (13-8) arise from the regions where t —> oo, only the asymptotic form of tfif need be considered in the evaluation of the integral. Furthermore since 4linear combination of atomic orbitals, eq. (13-8) becomes a sum of integrals ... [Pg.290]

Energy of Zero-Point-Motion is calculated for each nucleus rather than estimated or ignored. (3) Elaborate shape definitions are replaced by a matching procedure where the fragment interaction has the correct asymptotic form. (4) Microscopically calculated mass paramater functions are employed in two-dimensional action integrals. Mass asymmetry as well as charge asymmetry are fully taken into account. [Pg.97]

This formula expresses the surface integral obtained by integrating the kinetic energy integral by parts for open-channel orbital functions of the specified asymptotic form. In matrix notation,... [Pg.137]

The asymptotic form of the radial functions j/ (R) determines the matrix elements of the scattering matrix, Sjljri,. These in turn define the state-to-state integral and... [Pg.92]

Therefore, the integral term of (1.188) must become independent of y at large x. Since y tends to zero in the limit of large x, the lower limit of the integration may be replaced by zero. We thus find that the asymptotic form y(x) satisfies... [Pg.40]

For small t this is again just (1 - r kTIt). For larger t it approaches zero from below. Gordon has shown that successive integration by parts yields the useful asymptotic form... [Pg.29]

Clearly, the simplified form of is only valid for almost neutral molecules. In the case of strongly polar molecules and ions, the last term of Eq. (6.14) has to be taken into account, at least through its long-range components j%i. It may be remarked that if one introduces the two-center Coulomb integrals in their asymptotic form... [Pg.92]

Here y is Euler s constant, y = 0.57721566490.. . . The exponential integral function has a useful asymptotic form for small time scale and is given b... [Pg.252]

The exponential integral function, Eif(x), has an asymptotic form for small systems or long times, given by... [Pg.252]

Solution of the scattering amplitude may then be determined from the asymptotic form of i ( >j(iirectly from the integral representation... [Pg.2029]

Both of these integrals have obvious asymptotic forms. If the nucleus A in eqn (31.1) is very remote from the charge distribution then we may replace... [Pg.356]

In a completely analogous way, if the two charge distributions in eqn (31.2) are remote from each other the electron-repulsion integral has the asymptotic form... [Pg.356]

Again, if i = j and k = the electron-repulsion integral takes on the simple point-charge asymptotic form of 1/R, where this time R is the distance between the centroids of the two distributions. Since the basis functions are always atom-centred functions, the centroid of the diagonal charge distributions pu) are the relevant atoms and so the distances R are actually inter-atomic distances. [Pg.356]

The other extreme for the amount of electron in a charge distribution is zero when the two basis functions are orthogonal (5y = 0). In this case the asymptotic form for both types of integral is zero. [Pg.356]


See other pages where Integrals asymptotic forms is mentioned: [Pg.283]    [Pg.60]    [Pg.60]    [Pg.59]    [Pg.295]    [Pg.343]    [Pg.91]    [Pg.147]    [Pg.148]    [Pg.153]    [Pg.214]    [Pg.387]    [Pg.601]    [Pg.275]    [Pg.38]    [Pg.80]    [Pg.632]    [Pg.226]    [Pg.42]    [Pg.133]    [Pg.343]    [Pg.483]    [Pg.162]    [Pg.48]    [Pg.120]    [Pg.514]    [Pg.59]    [Pg.506]   
See also in sourсe #XX -- [ Pg.688 ]




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