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Paired states of fermions in two dimensions with breaking of parity
Paired states of fermions in two dimensions with breaking of parity

... In this paper we will make extensive use of the methods for BCS paired states, and consider the transitions between the weak and strong coupling regimes in two dimensions. In the weak-coupling regime, exotic phenomena are possible when parity and time reversal are broken. The results are applied to ...
Electric field control of magnetic anisotropy and domain wall motion
Electric field control of magnetic anisotropy and domain wall motion

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Quantum Information Technology based on Single Electron Dynamics
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Gas Ejection from Spiral Galaxy Disks Jeremy Durelle
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... We present the results of three proposed mechanisms for ejection of gas from a spiral arm into the halo. The mechanisms were modelled using magnetohydrodynamics (MHD) as a theoretical template. Each mechanism was run through simulations using a Fortran code: ZEUS-3D, an MHD equation solver. The firs ...
Electric field control of magnetism using BiFeO3
Electric field control of magnetism using BiFeO3

Lecture Notes in Statistical Mechanics and Mesoscopics Doron Cohen
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... Later we shall define some other ”spectral” functions that are related to H. Those can be written as an expectation value of functions of H. ...
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High- Energy Halo

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Chapter 2 Coulomb’s Law

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Physical mechanism of spontaneous fast reconnection evolution M. Ugai

... for the case of VC0 = 12(α = 0.5) during the nonlinear saturation phase of the fast reconnection evolution (Fig. 2), where a pair of thin current layers indicate slow (switch-off) shocks (here, the computational region is restricted to the first quadrant only because of the conventional symmetry bou ...
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effect of electron-electron correlation on the nonsequential

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Polaronic exciton in a parabolic quantum dot

Wizard Test Maker - Physics2010
Wizard Test Maker - Physics2010

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Physics Formulary

... possible corrections to the physics formulary. This document is Copyright 1995, 1998 by J.C.A. Wevers. All rights are reserved. Permission to use, copy and distribute this unmodified document by any means and for any purpose except profit purposes is hereby granted. Reproducing this document by any ...
Dissipative Quantum Systems with Potential Barrier. General
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Equilibrium concentration of point defects in crystalline
Equilibrium concentration of point defects in crystalline

Special Focus: Electrostatics - AP Central
Special Focus: Electrostatics - AP Central

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Aharonov–Bohm effect

The Aharonov–Bohm effect, sometimes called the Ehrenberg–Siday–Aharonov–Bohm effect, is a quantum mechanical phenomenon in which an electrically charged particle is affected by an electromagnetic field (E, B), despite being confined to a region in which both the magnetic field B and electric field E are zero. The underlying mechanism is the coupling of the electromagnetic potential with the complex phase of a charged particle's wavefunction, and the Aharonov–Bohm effect is accordingly illustrated by interference experiments.The most commonly described case, sometimes called the Aharonov–Bohm solenoid effect, takes place when the wave function of a charged particle passing around a long solenoid experiences a phase shift as a result of the enclosed magnetic field, despite the magnetic field being negligible in the region through which the particle passes and the particle's wavefunction being negligible inside the solenoid. This phase shift has been observed experimentally. There are also magnetic Aharonov–Bohm effects on bound energies and scattering cross sections, but these cases have not been experimentally tested. An electric Aharonov–Bohm phenomenon was also predicted, in which a charged particle is affected by regions with different electrical potentials but zero electric field, but this has no experimental confirmation yet. A separate ""molecular"" Aharonov–Bohm effect was proposed for nuclear motion in multiply connected regions, but this has been argued to be a different kind of geometric phase as it is ""neither nonlocal nor topological"", depending only on local quantities along the nuclear path.Werner Ehrenberg and Raymond E. Siday first predicted the effect in 1949, and similar effects were later published by Yakir Aharonov and David Bohm in 1959. After publication of the 1959 paper, Bohm was informed of Ehrenberg and Siday's work, which was acknowledged and credited in Bohm and Aharonov's subsequent 1961 paper.Subsequently, the effect was confirmed experimentally by several authors; a general review can be found in Peshkin and Tonomura (1989).
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