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Entropy and temperature of a quantum Carnot engine
Entropy and temperature of a quantum Carnot engine

Quantum (Separation of Variables) - Physics | Oregon State University
Quantum (Separation of Variables) - Physics | Oregon State University

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College of Engineering and Computer Science Mechanical

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1 The Postulates of Quantum Mechanics

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Analytical total photo cross section for atoms

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Quantum motion of electrons in topologically distorted crystals

... of the ideal lattice and consequently leads to a breakdown of the Bloch theorem for electronic quantum states. Outside the core region of such topological defects the lattice locally looks perfect but globally is distorted at arbitrary distances from the core. One therefore expects that sufficiently ...
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The Gutzwiller Density Functional Theory - cond

... : matrix of variational parameters (in this lecture problem: ...
SU(3) Model Description of Be Isotopes
SU(3) Model Description of Be Isotopes

3.3 The time-dependent Schrödinger equation
3.3 The time-dependent Schrödinger equation

... Schrödinger equation, with eigenenergy E is also a solution of the time-dependent equation as long as we always multiply it by a factor exp  iEt /   If   r  is a solution of the time-independent Schrödinger equation, with eigenenergy E then   r, t     r  exp  iEt /   is a solution ...
A brief introduction to chiral perturbation theory
A brief introduction to chiral perturbation theory

8.514 Many-body phenomena in condensed matter and atomic
8.514 Many-body phenomena in condensed matter and atomic

... where c is a scaling factor. The relation of coherent states with the points in a classical phase space will be clarified below. Let us find the form of a coherent state in the q-representation, ψυ (q) = < q | υ >. As before, we use the units in which the length λ=1, and write ...
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On the role of the electron-electron interaction in two-dimensional

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Mixed-State Evolution in the Presence of Gain and Loss

... that gain and loss can be balanced without perturbing the system, is possible. If, on the other hand, a coherent implementation of gain and loss is not feasible, either because of fundamental quantum limits or current technological limits, then it is important to take into account additional effects ...
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Operator methods in quantum mechanics
Operator methods in quantum mechanics

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Quantum mechanics in more than one

Long-range Rydberg-Rydberg interactions in calcium, strontium and
Long-range Rydberg-Rydberg interactions in calcium, strontium and

... case in general. In particular, many of the eigenstates of Ĥ (6) vary with n1 and n2 , unlike the eigenstates of Ĥ (5) . The correspondence between even and odd values of K and the symmetry under the interchange of the states of atoms 1 and 2 is nonetheless the same. In general, the composition of ...
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L14alternative - Particle Physics and Particle Astrophysics

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theory of fermi-bose quantum liquids

Advanced Atomic, Molecular and Optical Physics
Advanced Atomic, Molecular and Optical Physics

... • Atoms are the best examples of quantum systems we have. • They can be prepared in very well defined states. • Their temporal evolution can be measured and manipulated. • Atomic physics experiments can be reproduced all over the world. • They deliver the most accurate results in any experimental sc ...
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A linear chain of interacting harmonic oscillators: solutions as a

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Dirac Notation 1 Vectors

Quantum Transport Theory in Heterostructure Devices
Quantum Transport Theory in Heterostructure Devices

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Perturbation theory (quantum mechanics)

In quantum mechanics, perturbation theory is a set of approximation schemes directly related to mathematical perturbation for describing a complicated quantum system in terms of a simpler one. The idea is to start with a simple system for which a mathematical solution is known, and add an additional ""perturbing"" Hamiltonian representing a weak disturbance to the system. If the disturbance is not too large, the various physical quantities associated with the perturbed system (e.g. its energy levels and eigenstates) can be expressed as ""corrections"" to those of the simple system. These corrections, being small compared to the size of the quantities themselves, can be calculated using approximate methods such as asymptotic series. The complicated system can therefore be studied based on knowledge of the simpler one.
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