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A Bird`s-Eye View of Density-Functional Theory
A Bird`s-Eye View of Density-Functional Theory

... This paper is the outgrowth of lectures the author gave at the Physics Institute and the Chemistry Institute of the University of São Paulo at São Carlos, Brazil, and at the VIII’th Summer School on Electronic Structure of the Brazilian Physical Society. It is an attempt to introduce density-funct ...
A Bird`s-Eye View of Density
A Bird`s-Eye View of Density

Condensed Matter Approaches to Quantum Gases
Condensed Matter Approaches to Quantum Gases

Atomistic description of wave function localization effects in InxGa1
Atomistic description of wave function localization effects in InxGa1

Part II - American Chemical Society
Part II - American Chemical Society

Schwinger-Dyson operator of Yang-Mills matrix models with ghosts and derivations of the graded shuffle algebra
Schwinger-Dyson operator of Yang-Mills matrix models with ghosts and derivations of the graded shuffle algebra

Applications of Resolutions of the Coulomb Operator in Quantum
Applications of Resolutions of the Coulomb Operator in Quantum

... blackbody radiation, gas discharge tube and cathode ray. Attempts to explain these experiments led to the discovery of a new concept of physics whereby energy levels are not continuous but discrete. During the 19th century and early 20th century, there were many renowned scientists including Boltzma ...
Nonlinear Schrödinger equation and
Nonlinear Schrödinger equation and

The Many- Worlds Interpreta tion of Quantum Mechanics
The Many- Worlds Interpreta tion of Quantum Mechanics

Dissociation of H in the energy region at the n state
Dissociation of H in the energy region at the n state

... All 3s and 3d configurations are dominated by attractive Van der Waals interaction, although the 3d configurations contain a small quadrupole term as well. In contrast, the strongest contributions to the 3p potentials are dipole interaction terms. The interaction is repulsive for the 3ps, excluding ...
Physics - Dr. Bhim Rao Ambedkar University, Agra
Physics - Dr. Bhim Rao Ambedkar University, Agra

Parameterization and orbital angular momentum of anisotropic
Parameterization and orbital angular momentum of anisotropic

PDF only - at www.arxiv.org.
PDF only - at www.arxiv.org.

Sum rule of the correlation function
Sum rule of the correlation function

... correlations in the neutron-proton (n-p) system, where there are both the two-particle scattering states and a bound state, i.e., a deuteron. We prove that in spite of the attractive interaction, the n-p correlation can be negative because of the deuteron formation. Although some qualitative feature ...
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Core organic chemistry

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Interference of Bose#Einstein Condensates†

chapter 7 multielectron atoms outline
chapter 7 multielectron atoms outline

Calculation of Dispersion Energies - Psi-k
Calculation of Dispersion Energies - Psi-k

... fragments to the calculation of the (imaginary) frequency-dependent dipolar polarizability A of each fragment. This is a surprisingly demanding task. It can be done accurately with high-level quantum chemical approaches, but even relatively sophisticated treatments like RPA or ALDA obtain accuracies ...
M. Sc. Semester -I CHE401 Inorganic Chemistry
M. Sc. Semester -I CHE401 Inorganic Chemistry

Relativistic Effects in Atomic Spectra
Relativistic Effects in Atomic Spectra

... When quantum mechanics was emerging, new phenomena and paradoxes have occurred and one-particle systems needed to be discussed anew. Today, in quantum field theory or string theory representing modern physics, we are not even sure about the vacuum. In this thesis we investigate relativistic effects ...
The Path Integral Approach to Quantum Mechanics
The Path Integral Approach to Quantum Mechanics

3.3 The time-dependent Schrödinger equation
3.3 The time-dependent Schrödinger equation

... We know that if the potential V is constant in time each of the energy eigenstates  n  r  with eigenenergy En is separately a solution of the time-dependent Schrödinger equation provided we remember to multiply by the right complex exponential factor ...
Exact Conservation Laws of the Gradient Expanded Kadanoff–Baym
Exact Conservation Laws of the Gradient Expanded Kadanoff–Baym

Theoretical Studies on Kinetics of Molecular Excited States Feng
Theoretical Studies on Kinetics of Molecular Excited States Feng

... non-radiative transitions (intersystem crossing and internal conversion) in molecular and bio-related systems. One- or multi- dimensional potential energy surfaces (PESs) not only provide qualitative mechanistic explanation for excited state decay, but also make it possible to perform kinetic simula ...
Spin-Orbit Interactions in Topological Insulators
Spin-Orbit Interactions in Topological Insulators

< 1 ... 7 8 9 10 11 12 13 14 15 ... 68 >

Coupled cluster

Coupled cluster (CC) is a numerical technique used for describing many-body systems. Its most common use is as one of several post-Hartree–Fock ab initio quantum chemistry methods in the field of computational chemistry. It essentially takes the basic Hartree–Fock molecular orbital method and constructs multi-electron wavefunctions using the exponential cluster operator to account for electron correlation. Some of the most accurate calculations for small to medium-sized molecules use this method.The method was initially developed by Fritz Coester and Hermann Kümmel in the 1950s for studying nuclear physics phenomena, but became more frequently used when in 1966 Jiři Čížek (and later together with Josef Paldus) reformulated the method for electron correlation in atoms and molecules. It is now one of the most prevalent methods in quantum chemistry that includes electronic correlation.CC theory is simply the perturbative variant of the Many Electron Theory (MET) of Oktay Sinanoğlu, which is the exact (and variational) solution of the many electron problem, so it was also called ""Coupled Pair MET (CPMET)"". J. Čížek used the correlation function of MET and used Goldstone type perturbation theory to get the energy expression while original MET was completely variational. Čížek first developed the Linear-CPMET and then generalized it to full CPMET in the same paper in 1966. He then also performed an application of it on benzene molecule with O. Sinanoğlu in the same year. Because MET is somewhat difficult to perform computationally, CC is simpler and thus, in today's computational chemistry, CC is the best variant of MET and gives highly accurate results in comparison to experiments.
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