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XAS

Schomaker-StevensoD equation The equation a B = a + fl 0 09 (Xa - X ) relating the bond length to the individual radii rp and Tb of the two atoms concerned and the electronegativities Xp and X of the two atoms concerned in the bond. This relation is only empirical and is not very accurate. [Pg.353]

During inspection imaging processing features are used to observe details of the image. After inspection the images are stored on a CD ROM/XA diskette. [Pg.456]

Real Time X-Ray images are stored on CD ROM/XA. Compared to film the volume for a storage is reduced by a factor 50. Retrieving is easy since information of the location is given in the directory of the diskette. Normally the directory name is the shop order and the file name is the serial number of the part. The directory and file names can be customised. [Pg.457]

Figure la Schematic diagram of the experimental device axial translation of length Xa... [Pg.661]

The deviation of Gibbs monolayers from the ideal two-dimensional gas law may be treated by plotting xA// 7 versus x, as shown in Fig. III-15c. Here, for a series of straight-chain alcohols, one finds deviations from ideality increasing with increasing film pressure at low x values, however, the limiting value of unity for irAfRT is approached. [Pg.83]

Metals A and B form an alloy or solid solution. To take a hypothetical case, suppose that the structure is simple cubic, so that each interior atom has six nearest neighbors and each surface atom has five. A particular alloy has a bulk mole fraction XA = 0.50, the side of the unit cell is 4.0 A, and the energies of vaporization Ea and Eb are 30 and 35 kcal/mol for the respective pure metals. The A—A bond energy is aa and the B—B bond energy is bb assume that ab = j( aa + bb)- Calculate the surface energy as a function of surface composition. What should the surface composition be at 0 K In what direction should it change on heaf)pg, and why ... [Pg.286]

The projection of a domain plot onto its base makes a convenient two-dimensional graphical representation for describing adsorption-desorption operations. Here, the domain region that is filled can be indicated by shading the appropriate portion of the 45° base triangle. Indicate the appropriate shading for (a) adsorption up to Xa - 0.8 (b) such adsorption followed by desorption to Xd - 0.5 and (c) followed by readsorption from Xd = 0.5 to Xa = 0.7. [Pg.675]

Dunlap B I 1987 Symmetry and degeneracy in Xa and density functional theory Advances in Chemicai Physics vol LXIX, ed K P Lawley (New York Wiley-Interscience) pp 287-318... [Pg.2198]

Parr R G 1983 Density functional theory Ann. Rev. Phys. Chem. 34 631 -56 Salahub D R, Lampson S FI and Messmer R P 1982 Is there correlation in Xa analysis of Flartree-Fock and LCAO Xa calculations for O3 Chem. Phys. Lett. 85 430-3... [Pg.2198]

Becke A D 1983 Numerical Hartree-Fock-Slater calculations on diatomic molecules J. Chem. Phys. 76 6037 5 Case D A 1982 Electronic structure calculation using the Xa method Ann. [Pg.2199]

Seifert G, Eschrig FI and Bieger W 1986 An approximate variation of the LCAO-Xa method Z. Phys. Chem. 267 529... [Pg.2229]

Rdsch N, Sandl P, Gorling A and Knappe P 1988 Toward a chemisorption cluster model using the LCGTO-Xa method application to Ni(100)/Na Int. J. Ouantum Chem. Symp. 22 275... [Pg.2235]

The presented examples clearly demonstrate tliat a combination of several different teclmiques is urgently recommended for a complete characterization of tire chemical composition and tire atomic stmcture of electrode surfaces and a reliable interiDretation of tire related results. Stmcture sensitive metliods should be combined witli spectroscopic and electrochemical teclmiques. Besides in situ techniques such as SXS, XAS and STM or AFM, ex situ vacuum teclmiques have proven tlieir significance for tlie investigation of tlie electrode/electrolyte interface. [Pg.2755]

The elements of these vectors can be evaluated using an off-diagonal fomt of the Hellmann-Feynmann theorem, which in Cartesian coordinates, Xa, is... [Pg.278]


See other pages where XAS is mentioned: [Pg.176]    [Pg.151]    [Pg.275]    [Pg.385]    [Pg.657]    [Pg.657]    [Pg.657]    [Pg.657]    [Pg.265]    [Pg.265]    [Pg.405]    [Pg.624]    [Pg.642]    [Pg.668]    [Pg.714]    [Pg.716]    [Pg.26]    [Pg.153]    [Pg.154]    [Pg.591]    [Pg.1132]    [Pg.1470]    [Pg.2369]    [Pg.2524]    [Pg.2749]    [Pg.2751]    [Pg.2754]    [Pg.2754]    [Pg.210]    [Pg.424]    [Pg.427]    [Pg.429]    [Pg.432]    [Pg.432]   
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AlxGai xAs

Anti-factor Xa assay

Basic Principles of X-ray Absorption Spectroscopy (XAS)

Combination of XAS with Circular Dichroism in Metallomics and Metalloproteomics

DV-Xa method

DV-Xa molecular orbital calculation

Direct factor XA inhibitors

Discrete variational Xa method

Elastase, factors VIIa/TF, Xa, Xlla

Elastase, factors VIIa/TF, Xa, Xlla kallikrein

Factor Xa Inhibitors with Heterocyclic Moieties

Factor Xa inhibitors

In situ XAS

Inhibitors of factor Xa

LCGTO-Xa method

Modeling of XAS (EXAFS, XANES) Properties

Multiple scattering-Xa method

OF THE XAS

Ray absorption spectroscopy (XAS)

Relationship of XAS to Other Surface Science and in Situ Techniques

Relativistic DV-Xa method

SCF-Xa-SW calculation

Self-consistent field Xa scattered wave

Self-consistent field Xa scattered wave calculations

Slater Xa method

Slaters Multiple Scattering Xa Method for Molecules

Slaters Xa Model

Squash family serine protease inhibitor effects on Xa, Xlla, kallikrein

Survey of Published QSAR on Factor Xa Inhibitors

The Atomic Xa Model

The Difference Point (Xa)

The Xa Exchange Approximation

X-ray absorption spectroscopy XAS)

XA (mole fraction

XA state

XAS Measurement

XAS and Extended X-Ray Absorption Fine Structure (EXAFS) for Determination of the Short-Range Order

Xa Model

Xa Values

Xa approximation

Xa calculations

Xa exchange functional

Xa method

Xa multiple scattering

Xa scattered-wave method

Xa theory

Xa, Xlla, kallikrein, plasmin, trypsin

Xa-SW method

Xa-Scattered Waves

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