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A study on the derivation of a mean velocity formula from
A study on the derivation of a mean velocity formula from

An Overview of Impellers, Velocity Profile and Reactor
An Overview of Impellers, Velocity Profile and Reactor

... required data, it takes a long time to collect enough to build a model. In some cases, also it is difficult to obtain experimental information also. Pilot plant experiments can be considered as an option, but this conventional method has been left far behind by the advent of Computational Fluid Dyna ...
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Realizing effective magnetic field for photons by controlling the

... of the photon wavefunction. In ref. 23, this effect was then used to construct an optical isolator. An effective magnetic field, however, is characterized by the highly non-trivial topological properties of photon wavefunctions. In two dimensions, for example, one such topological property is a non-z ...
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... gap in the bulk and protected gapless modes on the boundary of the system[1, 2]. Integer quantum Hall states represent first examples of topologically protected phases in absence of any symmetries with the topological invariant directly related to the measured Hall conductance[3]. Recently, it becam ...
Path Integrals — Elementary Properties and Simple Solutions
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... the Trotter formula holds for operators which are bounded from below and that for most physically interesting potentials, it cannot be used to derive Feynman’s time-sliced path integral representation (2.14), even in systems where the formula is known to be valid. In particular, the short-time ampli ...
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11_abs_Fritz Riehle

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A New Perspective on Chiral Gauge Theories

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Hyperfine Splitting in Non-Relativistic Bound States Marc E. Baker

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Non-Equilibrium Liouville and Wigner Equations: Moment Methods

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On the adequacy of the Redfield equation and related approaches

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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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