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Ab initio Calculations of Optical Rotation
Ab initio Calculations of Optical Rotation

... When applicable, well-converged Gibbs free energy differences among confomers were determined using complete-basis-set extrapolations of CC energies in order to obtain Boltzmann-averaged specific rotations. The overall results indicate that the theoretical rotation is highly dependent on the choice ...
Ab initio embedded cluster study of optical second harmonic
Ab initio embedded cluster study of optical second harmonic

quantum field theory course version 03
quantum field theory course version 03

the atomic nucleus - NPAC
the atomic nucleus - NPAC

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Excitation of an Atomic Electron to a Coherent Superposition of

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Section 11.3 Atomic Orbitals

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Infinite-randomness quantum Ising critical fixed points

... is at zero quenched randomness. The second possibility is systems controlled by fixed points with nonzero, but finite, quenched randomness. In this case the coarsegrained behavior is spatially inhomogeneous, but the relative magnitude of the inhomogeneities remains finite at the fixed point. Example ...
Finite Element Method for Finite-Size Scaling in Quantum Mechanics
Finite Element Method for Finite-Size Scaling in Quantum Mechanics

... of a system when the size tends to infinity but a theory that also gives us numerical methods4–11 capable of obtaining accurate results for infinite systems by studying the corresponding small systems. Recently, we have applied the FSS theory to quantum systems.12–21 In this approach, the finite siz ...
Kazakov - From Sigma Models to Four-dimensional QFT
Kazakov - From Sigma Models to Four-dimensional QFT

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On the Time Evolution of Wavefunctions in Quantum Mechanics 1

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STATISTICAL FIELD THEORY

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Time propagation of extreme two-electron wavefunctions F Robicheaux

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The Action, The Lagrangian and Hamilton`s Principle

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Fock Matrix Construction for Large Systems

... As was mentioned in Section 2.2, the use of a single Slater determinant as an approximate wave function is known as the Hartree–Fock approximation. There are a few different variants of this approximation depending on how one treats the spins of the electrons that make up the Slater determinant. The ...
Hamiltonians Defined as Quadratic Forms
Hamiltonians Defined as Quadratic Forms

... is not always true. For example, if F is a square well with a zero energy 5-wave resonance, the integral equation has a solution for E = 0 but Hφ = 0 has no (square integrable) solutions. Whether a like occurrence can occur for E > 0 is an open question. ...
The Lamb shift in the hydrogen atom
The Lamb shift in the hydrogen atom

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Modified Schrödinger equation, its analysis and experimental

DEVIATIONS FROM EXPONENTIAL DECAY IN QUANTUM
DEVIATIONS FROM EXPONENTIAL DECAY IN QUANTUM

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4. Introducing Conformal Field Theory

Phonon-like excitations in the two-state Bose
Phonon-like excitations in the two-state Bose

Theoretical modeling of x-ray and vibrational spectroscopies applied to liquid
Theoretical modeling of x-ray and vibrational spectroscopies applied to liquid

The evolution of free wave packets
The evolution of free wave packets

Improper Schrodinger Equation and Dirac Equation
Improper Schrodinger Equation and Dirac Equation

5301-1.pdf
5301-1.pdf

... which can solve the Hartree–Fock equations for spin- 12 fermions moving in a three-dimensional (3D) harmonic oscillator potential, and interacting via delta-function potential. A basis set approach has been utilized in the program, in which the single-particle orbitals are expanded as a linear combi ...
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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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