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2015-2016 through 2016-2017
2015-2016 through 2016-2017

Notes on time dependence of wavefunctions
Notes on time dependence of wavefunctions

schrodinger
schrodinger

PowerPoint file of HBM_Intro _part I
PowerPoint file of HBM_Intro _part I

Core Ag Engineering Principles – Session 1
Core Ag Engineering Principles – Session 1

... the system used in the previous example was changed by removing a length of pipe and an elbow – what changes would that require you to make?  Would N1 change? D1? Q1? W1? P1?  Which direction (greater or smaller) would “they” move if they change? ...
Density profiles in open superdiffusive systems
Density profiles in open superdiffusive systems

Comparisons between classical and quantum mechanical
Comparisons between classical and quantum mechanical

... optical lattices generated by laser beams. This has already produced a number of fascinating results, but it has also proven to be an ideal test-ground for predictions from certain nonlinear lattice models. Because on the other hand, nonlinear science, the study of generic nonlinear phenomena, has i ...
Non-Equilibrium Quantum Many-Body Systems: Universal Aspects
Non-Equilibrium Quantum Many-Body Systems: Universal Aspects

... M. Eckstein, M. Kollar and P. Werner, Phys. Rev. Lett. 103, 056403 (2009); Phys. Rev. B 81, 115131 (2010) Non-equilibrium DMFT with real time QMC for interaction quench in half-filled Hubbard model ...
Nondimensionalization of equations
Nondimensionalization of equations

... the parameters present in the solution can be different from the dimensionless parameters present in the equations. Furthermore, from the latter, the former cannot be easily deduced, unless the same physical quantity is considered has having different dimensions when appearing in different physical ...
Percolation of Color Sources and the determination of the
Percolation of Color Sources and the determination of the

... measured value of the universal critical temperature Tc = 167.7 ± 2.6 MeV at the percolation threshold (ξc =1.2). The experimental value of the particle multiplicity density 3/2 dNc /dη, the average transverse momentum < pt > and the QE2 formation time τpro = 1.19 fm/c are used to convert the energy ...
Site-resolved imaging of a fermionic Mott insulator
Site-resolved imaging of a fermionic Mott insulator

Phys. Rev. Lett. 93, 073002
Phys. Rev. Lett. 93, 073002

... Raman photoassociation of 87 Rb atoms from a Mott insulator phase in an 3D optical lattice. By choosing appropriate parameters for the photoassociation laser fields, we have achieved control over both internal and external degrees of freedom of the molecules. A combination of Feshbach techniques and ...
American Journal of Physics, Vol. 71, Nº 1, 46-48 (2003).
American Journal of Physics, Vol. 71, Nº 1, 46-48 (2003).

A Primer on Quantum Mechanics and Orbitals
A Primer on Quantum Mechanics and Orbitals

... Where E is a number not a function (in this case total energy). Note that in equations like this after the application of the operator (in this case H, the Hamiltonian operator) to the wavefunction you get the eigenvalue (E) and the same wavefunction back. In the case we looked at above (the momentu ...
File - The Physics Doctor
File - The Physics Doctor

Fluid Mechanics Primer
Fluid Mechanics Primer

Chapter Four Fluid Dynamic
Chapter Four Fluid Dynamic

1 The Hamilton-Jacobi equation
1 The Hamilton-Jacobi equation

Calculation of the Masses of All Fundamental Elementary Particles
Calculation of the Masses of All Fundamental Elementary Particles

Proposal for Translational Entanglement of Dipole
Proposal for Translational Entanglement of Dipole

Hydrostatics and Bernoulli`s Principle Slide Notes
Hydrostatics and Bernoulli`s Principle Slide Notes

2. The Integer Quantum Hall Effect
2. The Integer Quantum Hall Effect

... A second reason why chiral modes are special is that it’s hard to disrupt them. If you add impurities to any system, they will scatter electrons. Typically such scattering makes the electrons bounce around in random directions and the net e↵ect is often that the electrons don’t get very far at all. ...
Experimental study of Bernoulli`s equation with losses
Experimental study of Bernoulli`s equation with losses

Chapter 5. The Schrödinger Wave Equation Formulation of Quantum
Chapter 5. The Schrödinger Wave Equation Formulation of Quantum

... Schrödinger’s version of quantum mechanics is based on the evolution of a wave function characterizing the system, a notion previously introduced in Chapter 4, as dictated by the Schrödinger wave equation. This is the approach we will take here. It is interesting to note, however, that Richard Feynm ...
Turbulence When the Reynolds number becomes sufficiently large
Turbulence When the Reynolds number becomes sufficiently large

... the same equation as laminar flow, but the effective (eddy) is much larger than its molecular value. When the mean velocity is zero, the momentum equation reduces to the diffusion equation with enhanced diffusivity. We argued above that the diffusivity for other quantities such as heat and salt shou ...
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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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