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Combinations of coefficients

The question is in the data from a real experiment, where many radionuclides are measured in many samples collected under a wide variety of conditions, what is the least number of classes of chemical behavior that will describe the observed results to the desired precision Or, in mathematical terms, what is the rank of the matrix A, and what nuclides should be selected to make up the submatrix a Finally, can any physical significance be attached to the combination of coefficients making up the elements of K, and can these elements of K or quantities thus derived be carried over from one event to the next ... [Pg.296]

The principal part of the eigenvectors, Ca, contains the combination of coefficients that is required to build Feynman-Dyson amplitudes (Dyson orbitals) from the reference Hartree-Fock orbitals. Dyson orbitals as they result from (1.12) are not normalized, i.e., the sum... [Pg.6]

Figure 12 Population transfer during precession (D) and exchanges (X) at the rth exchange. The population of basis coherences (see spots on lines) is transferred to eigencoherences (and vice versa) based on the linear combination of coefficients (spots on arrows). Colours black and grey have no meaning apart from making the alterations in the population of coherences visible. Figure 12 Population transfer during precession (D) and exchanges (X) at the rth exchange. The population of basis coherences (see spots on lines) is transferred to eigencoherences (and vice versa) based on the linear combination of coefficients (spots on arrows). Colours black and grey have no meaning apart from making the alterations in the population of coherences visible.
In standard degenerate perturbation theory,1 one forms a linear combination of degenerate states, and then selects the appropriate initial combination of coefficients. Likewise, in the present instance, we use the superposition theorem to write the wavefunction of a hybrid state - part discrete and part continuous - of energy E as ... [Pg.191]

The most widely used techmque for deriving QSAR equations is linear regression, which uses least-squares fitting to find the best combination of coefficients in the QSAR equation (the technique is also referred to as ordinary least-squares). We can illustrate the least-squares technique using the simple case where the activity is a function of just one property (when the technique is known as simple linear regression). We therefore want to derive an equation of the form ... [Pg.698]

If consideration is directed to processes rather than to species, the multiplicity (j) is the number of independent stoichiometric processes necessary to describe any arbitrary overall process. Then any possible combination of coefficients for which equation (T) is balanced can be generated by a linear combination of

independent component processes each of the form of equation (C). [Pg.61]

The representation of trial fiinctions as linear combinations of fixed basis fiinctions is perhaps the most connnon approach used in variational calculations optimization of the coefficients is often said to be an application of tire linear variational principle. Altliough some very accurate work on small atoms (notably helium and lithium) has been based on complicated trial functions with several nonlinear parameters, attempts to extend tliese calculations to larger atoms and molecules quickly runs into fonnidable difficulties (not the least of which is how to choose the fomi of the trial fiinction). Basis set expansions like that given by equation (A1.1.113) are much simpler to design, and the procedures required to obtain the coefficients that minimize are all easily carried out by computers. [Pg.38]

Alternatively, the electron can exchange parallel momentum with the lattice, but only in well defined amounts given by vectors that belong to the reciprocal lattice of the surface. That is, the vector is a linear combination of two reciprocal lattice vectors a and b, with integer coefficients. Thus, g = ha + kb, with arbitrary integers h and k (note that all the vectors a,b, a, b and g are parallel to the surface). The reciprocal lattice vectors a and are related to tire direct-space lattice vectors a and b through the following non-transparent definitions, which also use a vector n that is perpendicular to the surface plane, as well as vectorial dot and cross products ... [Pg.1768]

Furtlier details can be found elsewhere [20, 78, 82 and 84]. An approach to tire dynamics of nematics based on analysis of microscopic correlation fimctions has also been presented [85]. Various combinations of elements of tire viscosity tensor of a nematic define tire so-called Leslie coefficients [20, 84]. [Pg.2558]

MCSCF methods describe a wave function by the linear combination of M configuration state functions (CSFs), with Cl coefficients, Ck,... [Pg.300]

Note that the sums of the squares of the coefficients in a given MO must equal 1 (e.g., 0.3717 + 0.6015 + 0.3717 + 0.6015 = 1.0 for Pi) because each of the AOs represents a probability distribution of finding the electron at a given point in space. The total probability of finding an electron in all space for an MO must be unity, exactly as for its constituent AOs. We now can see that the LCAO approximation is only one of many possibilities to describe the electron density (= probability) for MOs. We do not have to express the electron density as a linear combination of the electron densities of AOs centered at the atoms. We could also... [Pg.378]

Fig. 3.13 Some of the possible combinations of atomic Is orbitals for a 2D square lattice corresponding to different values ofkj and ky. A shaded circle indicates a positive coefficient an open circle corresponds to a negative coefficient. Fig. 3.13 Some of the possible combinations of atomic Is orbitals for a 2D square lattice corresponding to different values ofkj and ky. A shaded circle indicates a positive coefficient an open circle corresponds to a negative coefficient.
The optimization procedure is canied out to find the set of coefficients of the eigenvector that minimizes the energy. These are the best coefficients for the chosen linear combination of basis functions, best in the sense that the linear combination of arbitrarily chosen basis functions with optimized coefficients best approximates the molecular orbital (eigenvector) sought. Usually, some members of the basis set of funetions bear a eloser resemblanee to the true moleeular orbital than others. If basis function a +i. [Pg.203]

Each of these factors can be viewed as combinations of CSFs with the same Cj and Cyj coefficients as in F but with the spin-orbital involving basis functions that have been differentiated with respect to displacement of center-a. It turns out that such derivatives of Gaussian basis orbitals can be carried out analytically (giving rise to new Gaussians with one higher and one lower 1-quantum number). [Pg.511]

All molecular orbitals are combinations of the same set of atomic orbitals they differ only by their LCAO expansion coefficients. HyperChem computes these coefficients, Cp , and the molecular orbital energies by requiring that the ground-state electronic energy be at a minimum. That is, any change in the computed coefficients can only increase the energy. [Pg.43]

Traditionally, production of metallic glasses requites rapid heat removal from the material (Fig. 2) which normally involves a combination of a cooling process that has a high heat-transfer coefficient at the interface of the Hquid and quenching medium, and a thin cross section in at least one-dimension. Besides rapid cooling, a variety of techniques are available to produce metallic glasses. Processes not dependent on rapid solidification include plastic deformation (38), mechanical alloying (7,8), and diffusional transformations (10). [Pg.336]


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Linear combination of atomic orbitals coefficients

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