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Applications space electronics

Roos B O 1987 The complete active space self-consistent field method and its applications in electronic structure calculations Adv. Chem. Phys. 69 399-445... [Pg.2200]

Applications of electron propagator methods with a single-determinant reference state seldom have been attempted for biradicals such as ozone, for operator space partitionings and perturbative corrections therein assume the dominance of a lone configuration in the reference state. Assignments of the three lowest cationic states were inferred from asymmetry parameters measured with Ne I, He I and He II radiation sources [43]. [Pg.47]

Kirtman B (1999) Local Space Approximation Methods for Correlated Electronic Structure Calculations in Large Delocalized Systems that are Locally Perturbed. 203 147-166 Klopper W, Kutzelnigg W, Muller H, Noga J, Vogtner S (1999) Extremal Electron Pairs - Application to Electron Correlation, Especially the R12 Method. 203 21-42 Knochel P, see Betzemeier B (1999) 206 61-78 Kozhushkov SI, see de Meijere A (1999) 201 1 -42... [Pg.198]

K. P. Lawley, Ed., chapter 69,399. John Wiley Sons Ltd., Chichester, England, 1987. The Complete Active Space Self-Consistent Field Method and its Applications in Electronic Structure Calculations. [Pg.280]

Information content in a powder diffraction pattern is reduced as compared to that in single crystal diffraction, due to the collapse of the three dimensional reciprocal space into a one dimensional space where the only independent variable is the scattering angle. The poorer the resolution of the diffraction method, the less the information content in the pattern (Altomare et al. 1995 David 1999). As a consequence, structure of less complex phases can be determined from power diffraction alone (fewer atoms in the asymmetric unit of the unit cell). However, refinement of the structure is not limited so seriously with resolution issues, so powder diffraction data are used in Rietveld refinement more frequently than in structure determination. Electron powder diffraction patterns can be processed and refined using public domain computer programs. The first successful applications of electron diffraction in this field were demonstrated on fairly simple structures. [Pg.194]

B. O. Roos, The Complete Active Space Self-Consistent Field Method and Its Application in Electronic Structure Calculation, Volume 69 olAdvances in Chemical Physics, Wiley, Chichester, 1987, p. 399. [Pg.381]

The PEMFC is nowadays the most advanced low-temperature fuel cell technology [19, 20], because it can be used in several applications (space programs, electric vehicles, stationary power plants, auxiliary power units, portable electronics). The progress made in one application is greatly beneficial to the others. [Pg.18]

B.O.Roos, The Complete Active Space Self-Consistent Field Method and its Application in Electronic Structure Calculations. [Pg.254]

Riplinger, C., Kao, J. P. Y., Rosen, G. M., Kathirvelu, V., Eaton, G. R., Eaton, S. S., Kutateladze, A., and Neese, F. (2009). Interaction of radical pairs through-bond and through-space Scope and limitations of the point-dipole approximation in electron paramagnetic resonance spectroscopy. J. Am. Chem. Soc. 131, 10092—10106. Schiemann, O., and Prisner, T. F. (2007). Applications of electron paramagnetic resonance to distance measurements in biomolecules. Q. Rev. Biophys. 40, 1—53. [Pg.350]

The Schrodinger wave equation15 is generally thought to contain, at least in principle, the solution to all chemical problems unfortunately it is wrong, or at least not universally valid,16 in the sense that Newton s Laws of Motion are valid but are not applicable to electrons and protons. The problem is that it is non-relativistic, that is, it does not treat space and time in... [Pg.23]

The Fourier transform equations show that the electron density is the Fourier transform of the structure factor and the structure factor is the Fourier transform of the electron density. Examples are worked out in Figures 6.14 and 6.15. If the electron density can be expressed as the sum of cosine waves, then its Fourier transform corresponds to the sum of the Fourier transforms of the individual cosine waves (Figure 6.16). The inversion theorem states that the Fourier transform of the Fourier transform of an object is the original object, hence the opposite signs in Equations 6.12.1 and 6.12.2. This theorem provides the possibility of using a mathematical expression to go back and forth between reciprocal space (structure factors) and real space (electron density), so that the phrase and vice versa is applicable here. [Pg.201]

The means for improving the real space, electron density map may involve a combination of ideas, but by far the most powerful is application of noncrystallographic symmetry. If the asymmetric unit contains noncrystallographic symmetry, then its electron density map does as well. If the dispositions of the noncrystallographic symmetry operators are known, then the electron density map can be self-averaged using these operators. [Pg.187]

Major polymer applications aerospace, electronics (mostly films and coatings), photosensitive materials for positive imaging, solar cells, hollow fiber membranes, composites. unclear power plants, space shuttle, microprocessor chip carriers, structural adhesives... [Pg.656]

THE COMPLETE ACTIVE SPACE SELF-CONSISTENT FIELD METHOD AND ITS APPLICATIONS IN ELECTRONIC STRUCTURE CALCULATIONS... [Pg.399]

The similarity indices S b(k) are also in the range 0-100%. Higher values imply greater similarity. An expression of this type was first discussed in detail by Hodgkin and Richards [10]. If Pa(p) = mxpsip), R bCw) is invariant to the choice of (non-zero) m, whereas S b( ) is not. In this sense, values of Seisin) are less dominated by the shape of the p-space electron densities than are the values of Rab(> ) This tends to make the Hodgkin-like definition more appropriate than the Carb6-like definition for some p-space applications. [Pg.100]

In summary, our unconventional approach to molecular similarity, based on indices derived from momentum-space electron densities, appears to show considerable promise for a wide range of applications. Work on a wide range of applications, both biological and non-biological, is currently in progress and the results will be reported in due course. [Pg.110]


See other pages where Applications space electronics is mentioned: [Pg.162]    [Pg.720]    [Pg.832]    [Pg.495]    [Pg.26]    [Pg.111]    [Pg.295]    [Pg.352]    [Pg.109]    [Pg.294]    [Pg.3816]    [Pg.334]    [Pg.16]    [Pg.86]    [Pg.87]    [Pg.743]   


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