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Delta-functions

Thus the delta function is an infinitely narrow and infinitely tall function having the area under the curve equal to unity. It can be considered as the limit of a set of real continuous functions, such as those given by the Gaussian function g(x) in (B.16) in which a successively smaller value is assigned to the standard deviation a. Asa tends to zero, the properties of g(x) approach those of (jc) as defined by Equations (B.27) and (B.28). [Pg.300]

By making the change of variables x - u and a - x and recognizing that (x) is an even function, Equation (B.32) can be rewritten in the form [Pg.301]

Convoluting/(jc) with a delta function thus leaves the function/ ) unchanged. Such an operation leaving the operand unmodified is called the identity operation, as is the case when zero is added to a number or a matrix is multiplied with a unit matrix. [Pg.301]

The function g(x) is named impulse response of the system, because it is the response to an unit pulse 5(x) applied at =0 [2]. This unit impulse 5(x), also called Dirac impulse or delta-function, is defined as... [Pg.366]

The Boltzmann constant is ks and T the absolute temperature. — is the Dirac delta function. Below we assume for convenience (equation (5)) that the delta function is narrow, but not infinitely narrow. The random force has a zero mean and no correlation in time. For simplicity we further set the friction to be a scalar which is independent of time or coordinates. [Pg.265]

Consider a numerical solution of the Newton s differential equation with a finite time step - At. In principle, since the Newton s equations of motion are deterministic the conditional probability should be a delta function... [Pg.268]

We assume that the sequential errors are not correlated in time, we can write the probability of sampling a sequence of errors as the product of the individual probabilities. We further use the finite time approximation for the delta function and have ... [Pg.269]

The application in [24] is to celestial mechanics, in which the reduced problem for consists of the Keplerian motion of planets around the sun and in which the impulses account for interplanetary interactions. Application to MD is explored in [14]. It is not easy to find a reduced problem that can be integrated analytically however. The choice /f = 0 is always possible and this yields the simple but effective leapfrog/Stormer/Verlet method, whose use according to [22] dates back to at least 1793 [5]. This connection should allay fears concerning the quality of an approximation using Dirac delta functions. [Pg.321]

Vgiec and Vxc represent the electron-nuclei, electron-electron and exchange-correlation dionals, respectively. The delta function is zero unless G = G, in which case it has lue of 1. There are two potential problems with the practical use of this equation for a croscopic lattice. First, the summation over G (a Fourier series) is in theory over an rite number of reciprocal lattice vectors. In addition, for a macroscropic lattice there effectively an infinite number of k points within the first Brillouin zone. Fortunately, e are practical solutions to both of these problems. [Pg.174]

Dirac delta function S Elution volume, exclusion Vo... [Pg.102]

In the opposite case of slow flip limit, cojp co, the exponential kernel can be approximated by the delta function, exp( —cUj t ) ii 2S(r)/coj, thus renormalizing the kinetic energy and, consequently, multiplying the particle s effective mass by the factor M = 1 + X The rate constant equals the tunneling probability in the adiabatic barrier I d(Q) with the renormalized mass M, ... [Pg.90]

Dirac delta function, an ideal pulse change ... [Pg.1087]

In the numerical solution the matrix structure is evaluated from Eqs. (44)-(46). Then Eqs. (47)-(49) with corresponding closure approximations are solved. Details of the solution have been presented in Refs. 32 and 33. Briefly, the numerical algorithm uses an expansion of the two-particle functions into a Fourier-Bessel series. The three-fold integrations are then reduced to sums of one-dimensional integrations. In the case of hard-sphere potentials, the BGY equation contains the delta function due to the derivative of the pair interactions. Therefore, the integrals in Eqs. (48) and (49) are onefold and contain the contact values of the functions... [Pg.333]

The von Niessen localization scheme uses the delta function of the distance between... [Pg.228]

A completely different type of property is for example spin-spin coupling constants, which contain interactions of electronic and nuclear spins. One of the operators is a delta function (Fermi-Contact, eq. (10.78)), which measures the quality of the wave function at a single point, the nuclear position. Since Gaussian functions have an incorrect behaviour at the nucleus (zero derivative compared with the cusp displayed by an exponential function), this requires addition of a number of very tight functions (large exponents) in order to predict coupling constants accurately. ... [Pg.262]

Letting Qn and p,i be the values of q and p just prior to the delta-function impulse, equations 4.42 may be integrated to yield the mapping... [Pg.193]

The time evolution of an arbitrary density pt=o x) may be obtained from equation 4.80 as follows. The Kronecker-delta function, 6 x — xq), evolves into the function 6 x — f xo)) after one step. Rewriting this in the form... [Pg.208]

Fig, 7,2 Spin-glass overlap probability Pspin-giaes(5) versus overlap q (equation 7,57) 6 x) is the Dirac-Delta function. [Pg.340]

In order to improve upon the mean-field approximation given in equation 7.112, we must somehow account for possible site-site correlations. Let us go back to the deterministic version of the basic Life rule (equation 7.110). We could take a formal expectation of this equation but we first need a way to compute expectation values of Kronecker delta functions. Schulman and Seiden [schul78] provide a simple means to do precisely that. We state their result without proof... [Pg.365]

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6 function delta Dirac distribution

An application of the Dirac delta function

Angular delta function

Appendix l.A — The Dirac Delta Function

Case of Delta-Function Barrier

Correlation delta-function

Delta

Delta function Fourier transform

Delta function computation

Delta function convolution with

Delta function distribution, catalyst activity

Delta function energy normalization

Delta function energy transfer

Delta function integral

Delta function multiplication

Delta function representation

Delta function response

Delta function, definition

Delta-function approximation

Delta-function properties

Dirac delta function

Dirac delta function approximation

Dirac delta function behavior

Dirac delta function energy-conserving

Dirac delta function integral representation

Dirac delta function matrices

Dirac delta function matrix elements

Dirac delta function models

Dirac delta function properties

Dirac delta function section

Dirac delta function spectral density

Dirac delta function three-dimensional

Dirac delta function transformations

Dirac delta function — Fourier transform

Dirac-delta function, catalyst

Dirac-delta function, optimal catalyst

Dirac’s delta function

Kronecker delta-function

Kronecker’s delta function

Separation distance delta function

Spectrum Dirac delta function

Total Dirac delta function

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