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CFD Introduction - Lyle School of Engineering
CFD Introduction - Lyle School of Engineering

A multiscale simulation environment for electronic and
A multiscale simulation environment for electronic and

Quantum Statistical Response Functions
Quantum Statistical Response Functions

Discrete vs continuous controversy in physics
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ThesisPresentation



... Since this is a 2-dimensional problem, there must be at least two quantum numbers which determine an energy state’s wave function and energy eigenvalue (one for each spatial coordinate). This is an important concept and has led us to find additional variables which effect a systems energy but which ...
Scattering Matrix Formulation of the Total Photoionization of Two
Scattering Matrix Formulation of the Total Photoionization of Two

... of two-electron atoms were at first explored from the viewpoint of the configuration interaction and the quantum defect theory [2,3]. Also, it was found that low-lying doubly-excited states could be labelled by approximate quantum numbers that could be understood in terms of group-theoretical quanti ...
Conservative, unconditionally stable
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PUBLISHED VERSION Quantum heat bath for spin-lattice
PUBLISHED VERSION Quantum heat bath for spin-lattice

The path integral representation kernel of evolution operator in
The path integral representation kernel of evolution operator in

Chapter 7 Fluorescence Imaging of Quantum Gases
Chapter 7 Fluorescence Imaging of Quantum Gases

results, conjectures and applications to quasicrystals
results, conjectures and applications to quasicrystals

... of translated ν (R) has a compact closure Ω which is called the Hull of R. The translation group Rd acts on Ω by homeomorphisms, so that (Ω, Rd ) defines a topological dynamical system. We will denote by τ a the translation by a ∈ Rd acting on Ω. It turns out that given any ω∈Ω one can find a unifor ...
Finite Volume Corrections to the Two
Finite Volume Corrections to the Two

Chemistry I/IH Chapter 9 Chemical Reactions Practice Test Multiple
Chemistry I/IH Chapter 9 Chemical Reactions Practice Test Multiple

Raman-induced oscillation between an atomic and a molecular
Raman-induced oscillation between an atomic and a molecular

The Time Dependent Schrödinger Equation
The Time Dependent Schrödinger Equation

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Computer simulated thermal energy atomic

... frame of quantum mechanics. The time dependent Schr odinger equation has been applied that corresponds to an initial value problem. This picture provides simple visualisation and physical interpretation. The physical space has been chosen large enough for containing the whole interaction region of ...
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approximation of thermal equilibrium for quantum gases with
approximation of thermal equilibrium for quantum gases with

... APPROXIMATION OF THERMAL EQUILIBRIUM FOR QUANTUM GASES ...
1 Derivation of Schrödinger`s equation Mikhail Batanov, Associate
1 Derivation of Schrödinger`s equation Mikhail Batanov, Associate

Trapping and Cooling Fermionic Atoms into Mott and - IPhT
Trapping and Cooling Fermionic Atoms into Mott and - IPhT

... lattice spacing, and 0 the chemical potential. We consider a mixture with equal number N=2 of " and # atoms. Experimentally the interaction parameter U and the hopping parameter J can be tuned independently changing the optical lattice height and using a Feshbach resonance. Note that the descriptio ...
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84, 085123 (2011)

Quantum vortices in a glass of Bose
Quantum vortices in a glass of Bose

Technical Report 2014-15 Lugre Tire Model for HMMWV
Technical Report 2014-15 Lugre Tire Model for HMMWV

Spin Angular Momentum and the Dirac Equation
Spin Angular Momentum and the Dirac Equation

... The divergence of displacement is ∂x ax + ∂y ay = 2(cos ϕ − 1), which is not zero in general. The theory of elastic waves could be improved by including higher-order deriatives, [8] but this does not solve the fundamental limitation to small displacements. Instead we use a different approach based on ...
< 1 ... 11 12 13 14 15 16 17 18 19 ... 48 >

Lattice Boltzmann methods

Lattice Boltzmann methods (LBM) (or Thermal Lattice Boltzmann methods (TLBM)) is a class of computational fluid dynamics (CFD) methods for fluid simulation. Instead of solving the Navier–Stokes equations, the discrete Boltzmann equation is solved to simulate the flow of a Newtonian fluid with collision models such as Bhatnagar-Gross-Krook (BGK). By simulating streaming and collision processes across a limited number of particles, the intrinsic particle interactions evince a microcosm of viscous flow behavior applicable across the greater mass.
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