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Vladimirov A.A., Diakonov D. Diffeomorphism
Vladimirov A.A., Diakonov D. Diffeomorphism

The lattice structure of quantum logics
The lattice structure of quantum logics

... projection postulate-unquestionable in the common opinion, but criticized by some prominent philosophers and theorists (e. g. [5]). The somewhat similar extension was previously discussed by the authors [3] on a quite different axiomatic basis. In the next section we collect our assumptions. They ar ...
Essentials of Modern Physics
Essentials of Modern Physics

... (h) extend the use of Bragg’s equation to electron diffraction in probing the surfaces of solids. (Only nonrelativistic cases are considered.) ...


On Quantum Sieve Approaches to the Lattice
On Quantum Sieve Approaches to the Lattice

The Kinetic Theory of Gases (2)
The Kinetic Theory of Gases (2)

... calories per mole, in agreement with the data shown in Figure 5.3 at low temperatures. Indeed, for all monatomic gases, the heat capacity per particle is cV = 32 kT . There is, however, much more to be explained about these diagrams, which are for diatomic molecules, and we will deal with these in d ...
Position Dependent Mass Quantum Particle - EMU I-REP
Position Dependent Mass Quantum Particle - EMU I-REP

Book Review: It Must Be Beautiful: Great Equations of Modern
Book Review: It Must Be Beautiful: Great Equations of Modern

Solutions of One-Dimensional Effective Mass Schrödinger Equation
Solutions of One-Dimensional Effective Mass Schrödinger Equation

CIEG-306 Fluid Mechanics Laboratory 5. HYDRAULIC JUMP
CIEG-306 Fluid Mechanics Laboratory 5. HYDRAULIC JUMP

Project 1: Computational Modeling of Flow and Surfactant Transport
Project 1: Computational Modeling of Flow and Surfactant Transport

Semiclassical approximation of excitations in spin-1 Heisenberg antiferromagnets
Semiclassical approximation of excitations in spin-1 Heisenberg antiferromagnets

The influence of effective mass on magnetoresistance in ultrathin Fe/Cr/Fe films K. W
The influence of effective mass on magnetoresistance in ultrathin Fe/Cr/Fe films K. W

QUANTUM LOGIC AND NON-COMMUTATIVE GEOMETRY
QUANTUM LOGIC AND NON-COMMUTATIVE GEOMETRY

... • The Baire*-algebras for bounded measurable observables make transparent the interpretation of quantum mechanics as a “theory of quantum probability” on a Topological NC phase space • As Streater pointed out: “Though the classical axioms were yet to be written down by Kolmogorov, Heisenberg, with h ...
a case against the first quantization
a case against the first quantization

Spin-1=2 Optical Lattice Clock
Spin-1=2 Optical Lattice Clock

Newton`s cradle analogue with Bose
Newton`s cradle analogue with Bose

Impact force of debris flow on filter dam
Impact force of debris flow on filter dam

1 Random Hamiltonians
1 Random Hamiltonians

Notes for Lecture 2 Miller Indices, Quantum Mechanics
Notes for Lecture 2 Miller Indices, Quantum Mechanics

A. Bylinkin - Rencontres de Moriond
A. Bylinkin - Rencontres de Moriond

... Good agreement with the Stefan-Boltzmann law for the Black Body radiation or the Bag model. Phys. Rev. C 90 (2014) 018201 A.A.Bylinkin et al. ...
Orthogonal polynomials, special functions and mathematical physics
Orthogonal polynomials, special functions and mathematical physics

... best suited to this model was the recently invented Hilbert space, where the basis was given by orthogonal polynomials [3]. The newly discovered orthogonal polynomials in the 20th century and the recently proposed multiple orthogonal polynomials open the door to new applications to more elaborate qu ...
Fokker-Planck theory of superstatistics
Fokker-Planck theory of superstatistics

Phys. Rev. Lett. 103, 025301 (2009).
Phys. Rev. Lett. 103, 025301 (2009).

... total number of particles and holes) and energy E in collinear processes. This conservation is exact for the modes gðn;EÞ , while it holds only to lowest order in  for gð Þ , being due to kinetic constraints on the two-body scattering of massless Dirac particles (see [28] for a related discussion). ...
2015-2016 through 2016-2017
2015-2016 through 2016-2017

< 1 ... 21 22 23 24 25 26 27 28 29 ... 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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