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K-matrix approach

A specific advantage of using the K-matrix approach in the present context is that the transition to a numerical treatment of the equations can be postponed until quite a late stage, thus allowing the full algebraic structure of the interacting resonances to be displayed. [Pg.248]

K-Matrix Approach The /C-matrix approach is based on an extension of Eq. (6.72) to matrix form... [Pg.244]

The CLS (also known as K-Matrix) approach is best applied to systems where the concentration of every... [Pg.592]

There are some limitations to the K-matrix approach. To obtain the matrix of concentration information, C must be inverted during the operations. This inversion demands that C be nonsingular requiring that there are no linear relationships between its component rows and columns. However, if rows or columns of the matrix have a linear relationship to each other, the determinant will be zero, the matrix singular, and noninvertable. This problem can be avoided by paying careful attention to the makeup of the calibrating standards. [Pg.127]

Another problem with the K-matrix approach occurs when the real samples contain impurities that are not in the standards. If an extra component appears in the region of analysis, it is possible to obtain a negative concentration in the unknown sample. [Pg.127]

Using GTO bases, it cannot be expected that the variational representations of the electron waves are snfficiently accnrate far ontside the so-called molecular region , i.e. the rather limited region of space where the potential clearly deviates from the asymptotic Conlomb form. Therefore the phaseshifts of the pwc basis states cannot be obtained from the analysis of their long-range behaviour, as was done in previous works with the STOCOS bases. In the present approach, this analysis may be avoided since the K-matrix techniqne allows to determine, by equation [3] below, the phase-shift difference between the eigenfunctions of Hp and the auxiliary basis functions... [Pg.369]

From this starting point, the authors develop equations leading to the evaluation of the real symmetric K matrix to specify the scattering process on the repulsive surface and propose its determination by a variational method. Furthermore, they show explicitly the conditions under which their rigorous equations reduce to the half-collision approximation. A noteworthy result of their approach which results because of the exact treatment of interchannel coupling is that only on-the-energy-shell contributions appear in the partial linewidth. Half-collision partial linewidths are found not to be exact unless off-the-shell contributions are accidentally zero or (equivalently) unless the interchannel coupling is zero. The extension of the approach to indirect photodissociation has also been presented. The method has been applied to direct dissociation of HCN, DCN, and TCN and to predissociation of HCN and DCN (21b). [Pg.102]

Levy, R. V., Souza, K. S., Neville, C. B. The matrix approach Microbial retention testing of sterilizing-grade filters with final parenteral products, part 1. Pharm Tech 14 161-173 (1990). [Pg.822]

P.G. Burke, K.A. Berrington, Atomic and Molecular Processes An R-matrix Approach, Institute of Physics, Bristol, 1993. [Pg.307]

Pfingst, K Nestmann, B.M. and Peyerimhoff, S.D. (1995). Tailoring the J -matrix approach for application to polyatomic molecules, in Computational Methods for Electron-Molecule Collisions, eds. W.M. Huo and F. Gianturco (Plenum,... [Pg.219]

Moszynski R, Jeziorski B, Rybak S, Szalewicz K, Williams HL (1994) Many-body theory of exchange effects in intermolecular interactions. Density matrix approach and applications to He-F-, He-HF, H2-HF, and Ar-H2 dimers. J Chem Phys 100 5080-5092... [Pg.135]

The matrix fracture behavior can also be described by using stress intensity factors, K. This approach is more convenient than the /-integral in some cases particularly for short cracks and for fatigue.31,84 To apply this approach, it is first necessary to specify the contribution to the crack opening induced by the applied stress, as well as that provided by the bridging fibers. For a plane strain crack of length 2a in an infinite plate, the contribution due to the applied stress is85... [Pg.40]

Varadan, V. K., "Multiple Scattering of Acoustic, Electromagnetic and Elastic Waves, Acoustic. Electromagnetic and Elastic Wave Scattering-Focus on the T-Matrix Approach. Pergamon Press, New York, 1980, pp. 103-134. [Pg.245]

Varadan, V. V. and Varadan, V. K., "Configuration with Finite Number of Scatterers — A Self Consistent T-Matrix Approach,"... [Pg.246]

Equations (2) and (3) outline the classical calibration and prediction approach and the combination is often referred to as K-matrix analysis. The K-matrix analysis approach requires quantitative calibration for all n components of the chemical system, even if they are of no interest for future predictions. Solution of equation... [Pg.26]

The model of chemical equilibrium is represented by the matrix N and vector K. Typical approach to the adsorption modeling can be described as follows. The Vy for solution species are usually known from literature, and the v,y for surface species have to be pre-assumed. The K, of solution species are usually known from literature, and the K, for surface species have to be fitted. The goal of the fitting procedure is to minimize Y in Eq, (5.11) for certain experimentally determined T and X. The method of solution of chemical equilibrium problem was discussed in detail by Herbelin and Westall [13], and many computer programs with user friendly interfaces are commercially available to perform this task. Once the fitting procedure is complete and the vector A is known, the Ad of the adsorbate, and its full speciation can be calculated for any experimental conditions (using the same... [Pg.587]

The calibration step in the CLS approach then involves the determination of the elements of the K matrix using the spectral data for a series of cahbration standards. For an n-component analysis, this involves the solution of a matrix equation of the form given in equation (18) ... [Pg.110]

The first part of the chapter contains a brief summary of Wigner s scattering theory, presented so as to emphasise the underlying similarity with the closely related approach of MQDT (chapter 3). This is followed by a discussion of the properties of S-, R- and K-matrices, in which we give the motivation for choosing one or the other, depending on the application in hand. Finally, we turn to some explicit applications of K-matrix theory to cases of interacting resonances in atomic physics. [Pg.247]

In principle, the correspondence between the two theories is not complete, because scattering theory is the more general formulation. For our purposes, however, the fact that the applications to atomic physics obtained by both methods are quite consistent with each other is an important and useful conclusion. The same result and connections have been obtained independently by Komninos and Nicolaides [378]. Both [373] and [378] noted that the derivation of MQDT from Wigner s scattering theory establishes its basic structure and theorems without special assumptions about the asymptotic forms of wavefunctions. The approach of Komninos and Nicolaides [378] is designed for applications involving Hartree-Fock and multiconfigurational Hartree-Fock bases. In the present exposition, we follow the approach and notation of Lane [379] and others [380, 381], who exploit the analytic K-matrix formalism and include photon widths explicitly when interferences occur. [Pg.248]

A fundamental issue in the description of even the simplest, isolated autoionising resonance in the parametric approach followed by Fano [391] - and further pursued in K-matrix theory - is that the atom cannot be deperturbed, that is one cannot access the so-called prediagonalised states which are imagined to exist prior to autoionisation being included as a perturbative interaction, since the effect is anyway internal to the atom and cannot truly be turned off. This has the disadvantage that the parameters, once they have been obtained, must still be calculated from an ab initio model of the atom for a full comparison with theory. It might seem that the parametric theory cannot really be checked independently of ab initio calculations whose accuracy is hard to ascertain. [Pg.265]

Mathematics of P and K Matrix Methods. Two basic forms of the matrix approach are in use, the so-called "K" and "P" matrix methods. Both methods involve using mixtures of known compositions as standards, then estimating concentrations in unknown mixtures using a set of calibration coefficients generated from the standard spectra. At each wavelength of the spectrum and for each calibration mixture, an extended form of Beer s law can be written as follows ... [Pg.369]

Real energy hermitian approaches. Extension of Fano s K-matrix, configuration interaction theory... [Pg.164]


See other pages where K-matrix approach is mentioned: [Pg.47]    [Pg.132]    [Pg.259]    [Pg.307]    [Pg.372]    [Pg.126]    [Pg.47]    [Pg.132]    [Pg.259]    [Pg.307]    [Pg.372]    [Pg.126]    [Pg.284]    [Pg.138]    [Pg.152]    [Pg.285]    [Pg.93]    [Pg.593]    [Pg.344]    [Pg.6]    [Pg.101]    [Pg.138]    [Pg.33]    [Pg.172]    [Pg.108]    [Pg.113]    [Pg.194]    [Pg.236]    [Pg.502]    [Pg.314]   
See also in sourсe #XX -- [ Pg.244 , Pg.245 ]




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K matrix

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