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Overlap integral volume

The last is known as the overlap integral as it is determined by the volume common to the atomic orbitals a and b at a given intemuclear distance. In general, 5 < 1, an integral that is often set equal to zero in approximate calculations. [Pg.372]

Autocorrelation Illustration. We choose a shape function Y (r) which describes a particle in 2D space (cf. Fig. 2.4a). Because of the definition of Y (r), T 2 (r) takes the value of the volume which is shared by the particle and its imagined ghost which is displaced by r. In any case the overlap integral becomes maximal for r = 0. Here the correlation is perfect. [Pg.35]

For small particles (R < as) the overlap integral I U(0) l of the electron and hole wave functions increases with decreasing nanoparticle volume as a result /is only weakly dependent on the particle size [113], However, volume normalized oscillator strength fA/) increases with decreasing nanoparticle size and can be estimated as [126] ... [Pg.237]

S is called the overlap integral because the integrand is only significant in regions of space where the charge distributions described by the AOs r and 0,v overlap. When either or or os is very small, the contribution to the integral from that volume element is small and so there are only substantial contributions from those regions of space where r and s overlap. A useful and speedy approximation is to invoke the zero overlap approximation (ZOA) which sets... [Pg.112]

Integral Sab is called the overlap integral. Physically it represents the common volume of the two atomic orbitals. A pictorial representation of Sab is given in Fig. 3.1.2. It is clear that Sab varies with rab, the internuclear distance when rab = 0, Sab = 1 when rab -> oo, Sab 0. Mathematically, it can be shown that, in a.u.,... [Pg.80]

A few of the characteristics of the integrals that need to be solved in the secular determinant should be outlined. Haa and Hbb are called coulomb integrals and are described as the energy of an electron occupying the basis orbital A or B. The resonance integral, Hab, is the quantum mechanical interaction term of basis orbital A with basis orbital B. 5ab is the overlap integral, the quantitative measure of the volume in space where the two basis functions interact. Basis functions that have zero overlap are said to be mutually orthogonal while two functions that are exactly coincident have an overlap value equal to 1 Saa = Sbb = 1, hence the simplification in the secular determinant above). In the secular determinant for the H2+ system or any homonuclear diatomic system, Haa = Hbb-... [Pg.2732]

W [(Vy n Vy) - Mo i,j)] + (1 - w) Mp i,j) where Mo(i, /) and Mp(i, j) are the common overlap steric volume and the integrated spatial difference in field potential, and w is a weighting factor between zero and one. The two descriptors are considered complementary in the sense that the overlap volume measures the shape within the van der Waals surface formed by superimposition of i and j, while ISDFP measures the shape outside the van der Waals surface. [Pg.325]

Equation (41a) means that the function B( r) is equivalent to the volume integral of the density matrix y(ri, ri) under the condition of r = r - r, and Eq. (41b) means that B(r) is the autocorrelation function of the position wave function (r). The latter is an application of the Wiener-Khintchin theorem (Jennison, 1961 Bracewell, 1965 Champeney, 1973), which states that the Fourier transform of the power spectrum is equal to the autocorrelation function of a function. Equation (41c) implies not only that B(r) is simply the overlap integral of a wave function with itself separated by the distance r (Thulstrup, 1976 Weyrich et al., 1979), but also that the momentum density p(p) and the overlap integral S(r) are a pair of the Fourier transform. The one-dimensional distribution along the z axis, B(0, 0, z), for example, satisfies... [Pg.193]

Before solving the determinant in equation 4.17, we will make some simplifying assumptions and approximations. The overlap integral, S, is a measure of the degree to which two orbitals occupy the same volume of space. It is not too difficult to see the rationale for assuming that Su = 1, since it is a property of normalized atomic orbitals that... [Pg.179]

As discussed in the previous section, all the possible interactions of o-Ps decrease its lifetime. The degree of this lifetime decrease is another parameter that can be related to physical and chemical properties of a system. The connection is quite obvious in the case of chemical reactions and ortho-para conversion. In the case of pick-off annihilation, the effects of the substance on positronium lifetime are expressed indirectly through the overlap integral in 0 Eq. (27.7). Any change in t/ v (e.g., changes of electron orbits) or in the overlap integral (e.g., free-volume changes) is reflected in the lifetime of o-Ps. [Pg.1472]

The only way for the differential overlap to be zero in Ju is for Xa or xb, or both, to be identically zero in dv. Zero differential overlap (ZDO) between Xa and xb in all volume elements requires that Xa and Xb can never be finite in the same region, that is, the functions do not touch. It is easy to see that, if there is ZDO between Xa and xb (understood to apply in all dv), then the familiar overlap integral S must vanish too. The converse is not tme, however. S is zero for any two orthogonal functions even if they touch. An example is provided by an s and a p function on the same center. [Pg.385]

The mathematical description of the model is out of the scope of this paper. Briefly, in this model, each reactant beam density is fitted to gaussian radial and temporal distribution functions, the spread in relative translational energy is neglected and the densities are assumed to be constant within the probed volume, which is smaller than the reaction zone. These assumptions result in a simple analytic expression of the overlap integral. Calculations are carried out for each rovibrational state of the outcoming molecule and for extreme velocity vector orientations, i.e, forwards and backwards. An example of the correction function, F, obtained for the A1 + O2 reaction at = 0.49 eV is displayed on Fig. 1, together with the... [Pg.108]

Table 1.5 Overlap integrals between molecular electron densities and overlap volumes for the nearest neighbor molecules iu the succiuic auhydride crystal. MP2/6-31G wavefimctiou... Table 1.5 Overlap integrals between molecular electron densities and overlap volumes for the nearest neighbor molecules iu the succiuic auhydride crystal. MP2/6-31G wavefimctiou...
Distance between centers of mass (A) Overlap integral (10-3 eA-3) Overlap volume at 0.002 eA 3 limit (A )... [Pg.20]

The corresponding overlap volume is the sum of the elementary volumes of all space pixels in which the electron density of both molecules is above a given threshold. The case is illustrated in Table 1.5 for the succinic anhydride crystal. As expected, the overlap integral correlates with the distance between molecular centers of mass. Coherently with the results shown in Table 1.4, the overlap volumes are non-zero only if the electron density threshold is less than 0.02 e A . In Section 12.2 it will be shown that the overlap integral correlates with the repulsion energy between neighbor molecules, and that the outer electrons play a crucial role in defining the details of the directional intermolecular interaction in crystals. [Pg.20]

Although based on integration over small volumes, the spin-pair composition yields a continuous function (i.e., the integration volumes overlap). In contrast, ELI is a discrete distribution of values, which formally can be made continuous in the so-called limit after rescaling (cf. Sect. 4). Formally, the spin-pair composition of Silvi could be seen as being based on the (/-restricted space partitioning, i.e., as ratio of same-spin and opposite-spin pairs in micro-cells enclosing fixed electron population. [Pg.133]

Micro Total Analysis Systems (pTAS) are chip-based micro-channel systems that serve for complete analytics. The word Total refers to the monolithic system character of the devices, integrating a multitude of miniature functional elements with minimal dead volumes. The main fields of application are related to biology, pharmacology, and analytical chemistry. Detailed applications of pTAS systems are given in Section 1.9.8. Recently, pTAS developments have strongly influenced the performance of organic syntheses by micro flow (see, e.g., [29]). By this, an overlap with the micro-reactor world was made, which probably will increase more and more. [Pg.16]


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