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Hermite form

Each of the methods described under rendering above can be applied directly to evaluation. The third, Hermite, form is probably most relevant to applications requiring high accuracy. In fact where the second derivative can also be evaluated exactly at dyadic points, a quintic Hermite interpolant can be used to give an even higher rate of approximation. [Pg.173]

The Hermite basis functions (p, t) have the following form ... [Pg.59]

There are infinitely many solutions and we assume that they are labelled according to their energies, Eq being the lowest. Since the H operator is Hermitic, the solutions form a complete basis. We may furthermore chose the solutions to be orthogonal and normalized. [Pg.407]

The Hermite polynomials Hn ) form an orthogonal set over the range —oo oo with a weighting factor e . If we equate coefficients of stY on each side of equation (D.12), we obtain... [Pg.299]

To determine the selection rules in this case it is sufficient to recall the relations developed in Section 5.S.1 between the Hermits polynomials. Specifically, Eq. (5-99) can be rewritten in the form... [Pg.369]

The two expansions discussed so far appear to be quite different. In the multistate Gaussian model, different functions are centered at different values of AU. In the Gram-Charlier expansion, all terms are centered at (AU)0. The difference, however, is smaller that it appears. In fact, one can express a combination of Gaussian functions in the form of (2.56) taking advantage of the addition theorem for Hermite polynomials [44], Similarly, another, previously proposed representation of Pq(AU) as a r function [45] can also be transformed into the more general form of (2.56). [Pg.65]

Here, the permutations of j, k,l,... include all combinations which produce different terms. The multivariate Hermite polynomials are listed in Table 2.1 for orders < 6. Like the spherical harmonics, the Hermite polynomials form an orthogonal set of functions (Kendal and Stuart 1958, p. 156). [Pg.32]

Two major forms of the OCFE procedure are common and differ only in the trial functions used. One uses the Lagrangian functions and adds conditions to make the first derivatives continuous across the element boundaries, and the other uses Hermite polynomials, which automatically have continuous first derivatives between elements. Difficulties in the numerical integration of the resulting system of equations occur with the use of both types of trial functions, and personal preference must then dictate which is to be used. The final equations that need to be integrated after application of the OCFE method in the axial dimension to the reactor equations (radial collocation is performed using simple orthogonal collocation) can be expressed in the form... [Pg.153]

This appendix gives some of the properties of the Hermite polynomials, HeN(jc). These polynomials form a basis set for Rahman s32 expansion of C s(v)(r, t) and play a fundamental role in the discussion of the non-Gaussian behavior of this latter function. Brief sketches of this expansion and of the... [Pg.162]

The Hermite polynomials Hn(g) form an orthogonal set over the range —oo oo... [Pg.299]

This is the important property of the Gaussian function, namely that its transform has the identical functional form as the original. This is called the property of self-reciprocity. All its derivatives also share the same property. The derivatives of the Gaussian function produce the well known Hermite functions. [Pg.79]

The absorption spectrum consists of sequences of transitions from v" = 0, 1, 2 to various v levels in the upper state, and the relative intensities of the vibration-rotation bands are given primarily by the product of the FCF value and a Boltzmann term, which can be taken to be exp — hcv v /kT). Common choices for the i/r s are harmonic oscillator and Morse wavefunctions, whose mathematical form can be found in Refs. 7 and 9 and in other books on quantum mechanics. The harmonic oscillator wavefunctions are defined in terms of the Hermite functions, while the Morse counterparts are usually written in terms of hypergeometric or Laguerre functions. All three types of functions are polynomial series defined with a single statement in Mathematica, and they can be easily manipulated even though they become quite complicated for higher v values. [Pg.80]

Hecht and Barron (1993) discuss the time reversal and Hermiticity characteristics of optical activity operators. They formulate the Raman optical activity observables for the four different forms of ROA in terms of matrix elements of the absorptive and dispersive parts of these operators. Rupprecht (1989) applied a matrix formalism for Raman optical activity to intensity sum rules. [Pg.569]

Hermite polynomials form part of the solution for the quantum mechanical treatment of the harmonic oscillator. One of these polynomials is defined by... [Pg.119]

A third form of symbiosis, in addition to mutualism and parasitism, is commensalism (Latin com = with mensa = table). In commensal relationships, one symbiotic partner benefits from the association and the other is unaffected. Different variants of snch relationships have been described. Inquilinism is a kind of commensalism where the symbiont uses a host for housing, snch as birds hving in the holes of trees. A more indirect dependency exists if a symbiont uses something its host has created before its death. This commensalism is termed metabiosis. A typical metabiont is the hermit crab that uses gastropod shells. In phoresy, the symbiont uses the host for transportation. An example for phoresy is the burdock, a plant with fruits that adhere to fur and are dispersed by the movement of mammals. [Pg.1747]

An operator with the property exhibited in eqn (5.5) is said to be Hermitian if it satisfies this equation for all functions P defined in the function space in which the operator is defined. The mathematical requirement for Hermiticity of H expressed in eqn (5.5) places a corresponding physical requirement on the system—that there be a zero flux in the vector current through the surface S bounding the system To illustrate this and other properties of the total system we shall assume, without loss of generality, a form for H corresponding to a single particle moving under the influence of a scalar potential F(r)... [Pg.138]


See other pages where Hermite form is mentioned: [Pg.65]    [Pg.65]    [Pg.65]    [Pg.65]    [Pg.21]    [Pg.155]    [Pg.262]    [Pg.317]    [Pg.58]    [Pg.61]    [Pg.161]    [Pg.399]    [Pg.591]    [Pg.2]    [Pg.134]    [Pg.150]    [Pg.249]    [Pg.391]    [Pg.216]    [Pg.96]    [Pg.724]    [Pg.159]    [Pg.445]    [Pg.12]    [Pg.12]    [Pg.40]    [Pg.44]    [Pg.341]    [Pg.96]    [Pg.724]    [Pg.208]    [Pg.145]   
See also in sourсe #XX -- [ Pg.64 ]




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