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Pth-order

Richardson extrapolation can be used to improve the accuracy of a method. Suppose we step forward one step At with a pth-order method. Then redo the problem, this time stepping foi ward from the same initial point, but in two steps of length Af/2, thus ending at the same point. Call the solution of the one-step calculation y and the solution of the two-step calculation yo. Then an improved solution at the new time is given by... [Pg.473]

Much of the recent literature on RDM reconstruction functionals is couched in terms of cumulant decompositions [13, 27-38]. Insofar as the p-RDM represents a quantum mechanical probability distribution for p-electron subsystems of an M-electron supersystem, the RDM cumulant formalism bears much similarity to the cumulant formalism of classical statistical mechanics, as formalized long ago by by Kubo [39]. (Quantum mechanics introduces important differences, however, as we shall discuss.) Within the cumulant formalism, the p-RDM is decomposed into connected and unconnected contributions, with the latter obtained in a known way from the lower-order -RDMs, q < p. The connected part defines the pth-order RDM cumulant (p-RDMC). In contrast to the p-RDM, the p-RDMC is an extensive quantity, meaning that it is additively separable in the case of a composite system composed of noninteracting subsystems. (The p-RDM is multiphcatively separable in such cases [28, 32]). The implication is that the RDMCs, and the connected equations that they satisfy, behave correctly in the limit of noninteracting subsystems by construction, whereas a 2-RDM obtained by approximate solution of the CSE may fail to preserve extensivity, or in other words may not be size-consistent [40, 42]. [Pg.262]

Here The quantity Q,p is called the pth-order energy density... [Pg.265]

Recall that the equation CSE(p) is written as r2p(l,1, =0, where Etp is the pth-order energy density matrix. Yasuda [11] has introduced a generating functional for the energy density matrices and used this functional to demonstrate that Qp = can be decomposed into a connected part... [Pg.282]

Certainly, we can took into account only a finite number of terms in the perturbation series (13). Let us assume that we perform calculations to the pth order of PT. If we use the M ller-Plesset PT then p < 4. The expression for AE2°" N) is easily obtained from Eqs. (19), (24), and (25)... [Pg.143]

Below we provide the relation of the pth moment to the pth-order commutator of H and T. In particular, we shall argue that the p = 0 moment, i.e., the normalization of the spectrum corresponds to the limiting short time information on the dynamics. Higher-order moments are seldom sufficient as the Taylor expansion... [Pg.20]

The values of k" and p are evaluated, and thence the value of the true rate constant, k, from knowledge of p, q, ub and the initial concentrations used. The kinetics given by equations (1-198) and (1-199) are said to be pseudo th- or pth-order in B and A, respectively. An example of this procedure is given in Figure 1.24 for a simple second-order reaction and, indeed, has already been explored somewhat in Illustration 1.9. In the figure example p = q = I the full process just described is not necessary however, the two experiments provide replicate measurements of k. [Pg.85]

The underlying nature of the problem is easy to comprehend (for an introductory geometric interpretation of these phenomena, see Crocker 1967, 1969). Interpreting the specific consequences in a particular problem can be extremely complicated. This is true because the ambiguity can be of up to Pth order. The problem is further complicated by the existence of two basic classes of intercorrelated ambiguity, which, for P 3, can simultaneously be present in all sorts of hierarchical combinations. Here, the surface will only be scratched with an illustration contrasting the two classes for P = 2, the least complex intercorrelation situation. (See also Sections 3.9 and 6.)... [Pg.2276]

We have presented the essence of the Runge-Kutta scheme, and now it is possible to generalize the scheme to a pth order. The Runge-Kutta methods are explicit methods, and they involve the evaluation of derivatives at various... [Pg.255]

Tensor of pth order represents 3 quantities Tyki... that are transformed, under the transformation of coordinate system x = ayXj, according to the law... [Pg.29]

Note 2 According to the definition of pth order tensor, scalars are zero-order tensors and vectors are first-order tensors. [Pg.30]

The left-hand side of Eq. (20) is reducible to an exponential integral function of the pth order, so the exact solution of the integral transcendental equation (23) for Ox can be obtained only by numerical methods and only if the function /f Ox) is known. Nevertheless, it follows from the general form of Eq. (23) that is independent of v and cfe and is determined only by the values ofp and aox- The latter is involved in Eq. (23) through ... [Pg.299]

Detailed analysis of the perturbation formulas reveals that the pth order correction to the wavefunction, cptp) jg actually sufficient to calculate all energy corrections up to (7p+ ) which is the content of the Wigner theorem. [Pg.1713]

Fig. 10.19 Isothermal effectiveness factor for reactions of pth order. (From TO. Salmi, J.-P. Mikkola, J.P. Warna, Chemical Reaction Engineering and Reactor Technology, 20i i, Boca Raton, FL Copyright 2011 CRC Press). Fig. 10.19 Isothermal effectiveness factor for reactions of pth order. (From TO. Salmi, J.-P. Mikkola, J.P. Warna, Chemical Reaction Engineering and Reactor Technology, 20i i, Boca Raton, FL Copyright 2011 CRC Press).

See other pages where Pth-order is mentioned: [Pg.265]    [Pg.178]    [Pg.441]    [Pg.459]    [Pg.342]    [Pg.126]    [Pg.57]    [Pg.58]    [Pg.254]    [Pg.124]    [Pg.1712]    [Pg.15]   


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