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Lecture Notes: Condensed Matter Theory I (TKM1)
Lecture Notes: Condensed Matter Theory I (TKM1)

... In addition, condensed matter physics is closely connected to materials science as well as mechanical, chemical, and electric engineering that focus on the design of novel materials and devices, ranging from better batteries, thermoelectric devices for waste heat conversion to superconductors, magne ...
Probing order beyond the Landau paradigm
Probing order beyond the Landau paradigm

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TRANSPORT PHENOMENA, FLOW OF FLUIDS A transport

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Chapter 10 Lattice Heat Capacity - Physics | Oregon State University
Chapter 10 Lattice Heat Capacity - Physics | Oregon State University

... solids to be dense, classical, ideal gases [see Eq.8.29] is in amazingly good agreement with the high temperature (∼ 300K ○ ) molar heat capacities of many solids, it fails to account for the observed rapid fall in cv at low temperature. An especially large effect in diamond caught Einstein’s (1907) ...
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ppt of slides

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Lecture Notes on Quantum Brownian Motion
Lecture Notes on Quantum Brownian Motion

Correction for housner`s equation of bending vibration of a pipe line
Correction for housner`s equation of bending vibration of a pipe line

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MULTIPLE CHOICE

A quantum random walk model for the (1 + 2) dimensional Dirac
A quantum random walk model for the (1 + 2) dimensional Dirac

Chapters 5-8 of SOURCEBOOK
Chapters 5-8 of SOURCEBOOK

... to many fields (especially in physics and chemistry) and by their nature can take substantial computing resources. • Note that the error in the computation only decreases like the square root of computer time used compared to the power convergence of most differential equation and particle dynamics ...
Chapter 1
Chapter 1

... positive energy levels. Likewise, it can never have zero energy, meaning that the particle can never "sit still". Additionally, it is more likely to be found at certain positions than at others, depending on its energy level. The particle may never be detected at certain positions, known as spatial ...
Heavy Ion Physics from RHIC to LHC Joe Kapusta
Heavy Ion Physics from RHIC to LHC Joe Kapusta

Lecture notes, Chapter 6. Time Evolution in Quantum Mechanics
Lecture notes, Chapter 6. Time Evolution in Quantum Mechanics

... (such as the probability density |ψ(x, t)|2 or the expectation values of observable, (A) = ψ(x, t)∗ A[ψ(x, t)]) are still time-independent. (Check it!) Thus we were correct in calling these states stationary and neglecting in practice their time-evolution when studying the properties of systems they ...
New Bloch Period for Interacting Cold Atoms in 1D Optical Lattices
New Bloch Period for Interacting Cold Atoms in 1D Optical Lattices

... crystal electron in an electric field). In this system, the effect of the field manifests in a very unintuitive way. Indeed, as already emphasized by Bloch [1] and Zener [2], according to the predictions of wave mechanics, the motion of electrons in a perfect crystal should be oscillatory rather tha ...
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Enthralled by symmetries

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The Free Particle

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Laminar and Turbulent Flow in Pipes

... The velocity profile in a pipe will show that the fluid at the centre of the stream will move more quickly than the fluid towards the edge of the stream. Therefore friction will occur between layers within the fluid. Fluids with a high viscosity will flow more slowly and will generally not support e ...
Chiral Spin States in the Pyrochlore Heisenberg Magnet
Chiral Spin States in the Pyrochlore Heisenberg Magnet

...  Fermionic mean-field theory and variational Monte Carlo techniques have been employed to understand the nature of the ground state of the spin-1/2 Heisenberg model on the pyrochlore lattice.  From VMC calculations, of the four different flux states considered, the [/2,/2,0]-flux state had the l ...
Relaxation dynamics of a quantum Brownian particle in an ideal gas
Relaxation dynamics of a quantum Brownian particle in an ideal gas

Full Text PDF
Full Text PDF

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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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