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Atomic application

In fact, the HF procedure leads to a complicated set of integro-differential equations that can only be solved for a one-centre problem. If your interest lies in atomic applications, you should read the classic books mentioned above. What we normally do for molecules is to use the LCAO procedure each HF orbital is expressed as a linear combination of n atomic orbitals X . Xn... [Pg.113]

All the complete sets mentioned here are referred to a certain origin and, in an atomic application, this point may conveniently be chosen to coincide with the nucleus. In a molecular problem, this problem is more difficult one may use a single complete set as in the united atom model, or one may introduce a complete set at every nucleus or at certain suitably chosen points ( floatingpoint wave functions). If more than one complete set is intro-... [Pg.276]

Daudel, R., Odiot, S., and Brion, H., Compt. rend. 238, 456, La notion de loge et la signification g6om6trique de la notion de couche dans le cortege electronique des atomes. The concept of box, the geometrical significance of the shell concept in the electron cloud of the atoms. Application to the He atom. [Pg.338]

B—Calcium Calcium anode N.G. N.G. Thermal batteries for military and atomic applications... [Pg.1310]

Levy, H. R., Talalay, P., Vennesland, B. The steric course of enzymatic reactions at meso carbon atoms application of hydrogen isotopes. In progress in stereochemistry (ed. de la Mare and Klyne), Vol. 3, p. 299—349. (London Butterworths 1962. [Pg.66]

D.D. Richardson, A calculation of Van der Walls interactions in and between layers of atoms application to graphite. J.Phys. C Solid State Phys., 10 (1977) 3235-3242. [Pg.317]

It should be remarked that this is the first practical implementation of the calculation of spin-spin couplings involving heavy atoms applicable to medium sized molecular systems. Formerly, Khandogin and Ziegler101 developed a frozen core scalar relativistic approach in combination with the non-relativistic FC and PSO operators, but the quality of results thus obtained is poorer than those obtained with ZORA. [Pg.181]

We see from this diagram that for the reaction of hydrogen and chlorine to form hydrogen chloride the two spans of zero length (for the two bonds H—H and Cl—Cl) are converted into two longer spans (for the two bonds II—Cl). (The word span is used to represent the difference in electronegativity of the two atoms.) Application of Equation 3-12 shows that such a reaction is predicted to be exothermic. [Pg.103]

Manson, J.R. and Ritchie, R.H. (1985). Completely quantal treatment of the van der Waals forces between atoms application to positronium. Phys. Rev. Lett. 54 785-788. [Pg.426]

The way in which the exclusion principle determines the order of hydrogenlike energy-level occupation in many-electron atoms, is by dictating a unique set of quantum numbers, n, /, mi and spin ms, for each electron in the atom. Application of this rule shows that the sub-levels with l = 0, 1, 2 can accommodate no more than 2, 6, 10 electrons respectively. In particular, no more than two electrons with ms = , can share the same value of mi. Each principal level accommodates 2n2 electrons. [Pg.58]

Calculations for Poly atomics Applications to PbH2, S11H2, and GeHj. [Pg.202]

For monoalkyl benzenes, there is evidence of a second mechanism for hydrocarbon decomposition. Since substantial amounts of benzalde-hyde (representing a 5-25% yield) and traces (< 1% yield) of peroxy-benzoyl nitrate have been identified (10) in smog chamber experiments with aromatic hydrocarbons having at least two benzylic hydrogens, hydrocarbon oxidation apparently may occur at the a-carbon atom. Application of the usual Hammett treatment and electrophilic substituent constants (23) to any of our rate measurements for toluene, fert-butyl-benzene, and benzene indicates no linear Hammett relationship toluene... [Pg.113]

The way in which the exclusion principle determines the order of hydrogen-like energy-level occupation in many-electron atoms is by dictating a unique set of quantum numbers, n, I, nii and m, for each electron in the atom. Application of... [Pg.463]

Here P and Q are the radial large and small components of the wavefunction, the angular functions are 2-component spinors, the quantum number k = 2 - j) j + 1/2), -j < rrij < j, and the phase factor i is introduced for convenience in some atomic applications because it makes the radial Dirac equation real. [Pg.261]

J. Maruani, A. Khoudir, M. Tronc, G. Giorgi and C. Bonnelle, A mediod of combined treatment for die evaluation of core ionization energies in molecules involving heavy atoms application to CrF6, MoF6 and WF6 , Int. J. Quant. Chem., to be submitted. [Pg.89]

Here total means that g(r) pertains to all the diffracting atoms. Application of x-ray diffraction results in the structure of liquid water, in terms of g(Ow-Ow, r), since only the oxygen atoms, but not the hydrogen atoms, diffract x-rays. This function resembles to some extent that of liquid argon, a non-structured liquid by aU accounts (Fisenko et al. 2008), as demonstrated by Marcus (1996). There is, thus, more in the notion of the structure of water than what is measurable by g(r), which is dominated by the strong repulsion of molecules that are too closely packed together. [Pg.8]

Since the mean-field spin-orbit integrals have been defined and implemented to molecular codes (Dalton, Molcas etc.), hundreds or more successful molecular and atomic applications have been performed with the accuracy comparable to the experimental results. [Pg.12]

When the chiral center is tricoordinate, as is the case for sulfoxides sulfonium salts, and phosphines, then a phantom atom of atomic number zero is taken to occypy the lowest-priority site of a presumed tetrahedral atom. Application of the sequence rule in the usual manner allows the assignment of the R configuration to the benzyl phenyl sulfoxide enantiomer and the 5 configuration to the methylal-lylphenylphosphine enantiomer shown in Scheme 2.1. [Pg.73]

Figure 5.3 Schematic representation of the dipole-dipole attraction that exists between the instantaneous dipoles of two atoms in two particles. The + represents the nucleus of the atom and the represents the centre of the electron density. Because the centre of electron density is t3 ically not coincident with the nucleus, a dipole moment exists between the two separated opposite charges in each atom. Application of Coulomb s law between the charges indicates that the lowest free energy configuration is as shown in the figure. The resulting position of positive and negative charges leads to an attraction between the two atoms, again due to Coulomb s law... Figure 5.3 Schematic representation of the dipole-dipole attraction that exists between the instantaneous dipoles of two atoms in two particles. The + represents the nucleus of the atom and the represents the centre of the electron density. Because the centre of electron density is t3 ically not coincident with the nucleus, a dipole moment exists between the two separated opposite charges in each atom. Application of Coulomb s law between the charges indicates that the lowest free energy configuration is as shown in the figure. The resulting position of positive and negative charges leads to an attraction between the two atoms, again due to Coulomb s law...
Kastler, A., 1950. Quelques suggestions concemant la production optique et la detection optique d une inegalite de population des niveaux de quantification spatiale des atomes. Application a I experience de Stem et Gerlach et a la resonance magnetique. J. Hiys. Radium 11, 255-265. [Pg.256]


See other pages where Atomic application is mentioned: [Pg.81]    [Pg.455]    [Pg.11]    [Pg.553]    [Pg.159]    [Pg.21]    [Pg.246]    [Pg.19]    [Pg.105]    [Pg.274]    [Pg.310]    [Pg.265]    [Pg.265]    [Pg.312]    [Pg.28]    [Pg.189]    [Pg.147]    [Pg.293]    [Pg.595]    [Pg.115]    [Pg.31]    [Pg.147]    [Pg.131]    [Pg.81]    [Pg.365]    [Pg.497]   
See also in sourсe #XX -- [ Pg.56 ]




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