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Electron total energy

Defining the true electronic total energy of the system as Eeiect =T+ -t- W and the total... [Pg.492]

Box 4. 4 orbitals 4 electrons Total Energy (Coulomb +Exchange) and Diabatic Surface Model... [Pg.270]

STM consists of a sharp metal tip that is placed over a conductive sample surface (Fig. 1). The conduction electrons are free to propagate within the tip and the sample, but classically forbidden in the gap between the tip and the sample in which the electron total energy is smaller than the potential energy. However, according... [Pg.758]

ONETEP [1], the order-N electronic total energy package is a numerical implementation of Density Functional Theory. Unlike usual implementations of DFT, the computational resources required for the calculation of the energy of a particular atomic system scales linearly with the number of electrons, which makes it exceptionally efficient in investigations of large systems. However, in our work we exploited another feature of ONETEP, namely, that it uses local basis functions. [Pg.60]

In this section, the ground state properties of the lanthanides are studied with a first principles all-electron total energy band structure method. The LMTO method is employed within the local density (LDA) and local spin density (LSD) functional approximations (Hohenberg and Kohn 1964, Kohn and Sham 1965, Gunnarsson and Lundqvist 1976). The von Barth-Hedin (1972) interpolation formula is used for the exchange and correlation potential with the parameters of Hedin and Lundqvist (1971) and RPA scaling (Janak 1978). [Pg.170]

Moreover, for the bonding stable states, the electrons total energy, seen as an electronic gas, is equivalent to -T (minus kinetic energy of electrons), by the virtue of the virial theorem. [Pg.210]

Then, since the electronic total energy is a negative measure (of minimum) of the stability of a structure, the relation (2.198) for electronic density will be controlled, eventually, by the topology (space distribution) of Laplacian (A) of electronic density, with minus sign, i.e.,-Ap r). On the other side, the fact that the VSEPR paradigm takes in consideration the electron pairs and not the individual electrons should be quantified, for which reason a particular measure for the inter-separation of the electron pairs will be introduced. [Pg.211]

FIGURE 5 Differential electron total energy distribution of the events produced by B solar neutrinos. The dashed histogram is the best fit to the data of a Monte Carlo calculation based on ff (vee ves), the known shape of the neutrino flux from B decay, and the energy resolution of the detector. The solid histogram has the shape dictated by the considerations above but the area predicted by the SSM in Bahcall and Ulrich (see Table III). [Pg.205]

If the increase in the total energy of a system of N conduction electrons when heated from zero to T is denoted by AU, then... [Pg.431]

Because NH has an electron affinity of 0.4 eV, the total energies of the above two states can be equal only if the kinetic energy KE carried away by the ejected electron obeys... [Pg.2156]

The orbitals from which electrons are removed can be restricted to focus attention on the correlations among certain orbitals. For example, if the excitations from the core electrons are excluded, one computes the total energy that contains no core correlation energy. The number of CSFs included in the Cl calculation can be far in excess of the number considered in typical MCSCF calculations. Cl wavefimctions including 5000 to 50 000 CSFs are routine, and fimctions with one to several billion CSFs are within the realm of practicality [53]. [Pg.2176]

This gives the total energy, which is also the kinetic energy in this case because the potential energy is zero within the box , m tenns of the electron density p x,y,z) = (NIL ). It therefore may be plausible to express kinetic energies in tenns of electron densities p(r), but it is by no means clear how to do so for real atoms and molecules with electron-nuclear and electron-electron interactions operative. [Pg.2181]

Once the requisite one- and two-electron integrals are available in the MO basis, the multiconfigurational wavefunction and energy calculation can begin. Each of these methods has its own approach to describing tlie configurations d),. j included m the calculation and how the C,.] amplitudes and the total energy E are to be... [Pg.2185]

QMC teclmiques provide highly accurate calculations of many-electron systems. In variational QMC (VMC) [112, 113 and 114], the total energy of the many-electron system is calculated as the expectation value of the Hamiltonian. Parameters in a trial wavefiinction are optimized so as to find the lowest-energy state (modem... [Pg.2220]

Figure B3.2.11. Total energy versus lattice constant of gallium arsenide from a VMC calculation including 256 valence electrons [118] the curve is a quadratic fit. The error bars reflect the uncertainties of individual values. The experimental lattice constant is 10.68 au, the QMC result is 10.69 (+ 0.1) an (Figure by Professor W Schattke). Figure B3.2.11. Total energy versus lattice constant of gallium arsenide from a VMC calculation including 256 valence electrons [118] the curve is a quadratic fit. The error bars reflect the uncertainties of individual values. The experimental lattice constant is 10.68 au, the QMC result is 10.69 (+ 0.1) an (Figure by Professor W Schattke).
Weinert M, Wimmer E and Freeman A J 1982 Total-energy all-electron density functional method for bulk solids and surfaces Phys. Rev. B 26 4571-8... [Pg.2235]

Jansen H J F and Freeman A J 1984 Total-energy full-potential linearized augmented plane-wave method for bulk solids electronic and structural properties of tungsten Phys. Rev. B 30 561-9... [Pg.2235]

For each configuration of the nuclei, minimization of tlie total energy with respect to the electron density yields the instantaneous value of a potential energy fiinction V(/ ), and the corresponding forces on the nuclei. In principle,... [Pg.2275]

A quantum mechanical treatment of molecular systems usually starts with the Bom-Oppenlieimer approximation, i.e., the separation of the electronic and nuclear degrees of freedom. This is a very good approximation for well separated electronic states. The expectation value of the total energy in this case is a fiinction of the nuclear coordinates and the parameters in the electronic wavefunction, e.g., orbital coefficients. The wavefiinction parameters are most often detennined by tire variation theorem the electronic energy is made stationary (in the most important ground-state case it is minimized) with respect to them. The... [Pg.2331]


See other pages where Electron total energy is mentioned: [Pg.313]    [Pg.193]    [Pg.156]    [Pg.178]    [Pg.175]    [Pg.257]    [Pg.193]    [Pg.1565]    [Pg.191]    [Pg.260]    [Pg.313]    [Pg.193]    [Pg.156]    [Pg.178]    [Pg.175]    [Pg.257]    [Pg.193]    [Pg.1565]    [Pg.191]    [Pg.260]    [Pg.714]    [Pg.32]    [Pg.89]    [Pg.92]    [Pg.96]    [Pg.137]    [Pg.1332]    [Pg.1466]    [Pg.2181]    [Pg.2181]    [Pg.2207]    [Pg.2208]    [Pg.2213]    [Pg.2218]    [Pg.2220]    [Pg.2223]    [Pg.2275]    [Pg.2322]    [Pg.81]    [Pg.214]    [Pg.400]   
See also in sourсe #XX -- [ Pg.10 , Pg.11 ]




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