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Electromagnetical model of an induction motor in COMSOL
Electromagnetical model of an induction motor in COMSOL

Spin Interactions Between Conduction Electrons and
Spin Interactions Between Conduction Electrons and

Martin Raith - Publikationsserver der Universität Regensburg
Martin Raith - Publikationsserver der Universität Regensburg

Shock and Discontinuity Normals, Mach Numbers, and Related
Shock and Discontinuity Normals, Mach Numbers, and Related

... flows and which effects an irreversible (i.e., entropy-increasing) transition via dissipation of some sort. At the macroscopic level, the shock must conserve total mass, momentum, and energy fluxes, together with an obeyance of Maxwell’s equations. Adopting a particular macroscopic framework, such a ...
Few-body interactions in an ultracold gas of Cesium atoms
Few-body interactions in an ultracold gas of Cesium atoms

Theoretical and observational consistency of Massive Gravity
Theoretical and observational consistency of Massive Gravity

... and study explicitly the stability of the graviton potential when including matter and graviton loops based on our work in de Rham et al.. The analysis of the one-loop matter quantum corrections reveals that the potential remains unaffected since they contribute only in form of a cosmological consta ...
chp-07 - WordPress.com
chp-07 - WordPress.com

Normandeau Associates et al. 2011
Normandeau Associates et al. 2011

... 3. Literature Search and Information Gathering Results (Task 1) ...............................................29 3.1 Existing and Proposed Undersea Power Cables ............................................................29 3.2 Magnetosensitive and Electrosensitive Marine Species .................. ...
Vortex Dynamics in Bose-Einstein Condensates
Vortex Dynamics in Bose-Einstein Condensates

TIME-REVERSAL INVARIANT TOPOLOGICAL INSULATORS A
TIME-REVERSAL INVARIANT TOPOLOGICAL INSULATORS A

Few-body physics in ultracold Fermi gases
Few-body physics in ultracold Fermi gases

... the quantum mechanical three-body problem which are necessary to understand the experiments and their interpretation described in the later course of this thesis. Efimov’s scenario which predicts an infinite number of bound states for resonant two-body interactions is discussed and important results ...
Tunneling from a correlated two-dimensional electron system transverse to a... * T. Sharpee and M. I. Dykman P. M. Platzman
Tunneling from a correlated two-dimensional electron system transverse to a... * T. Sharpee and M. I. Dykman P. M. Platzman

... a 2D wave vector k. We chose the equilibrium in-plane position of the tunneling electron to be at the origin. Then its in-plane 2D momentum is p⫽N ⫺1/2兺 pkj for B⫽0. The interaction Hamiltonian H B 共4兲 does not conserve the phonon quasimomentum k. The Hall momentum of the tunneling electron is trans ...
PDF 3.1 MB - Department of Physics
PDF 3.1 MB - Department of Physics

... times, the stimulating discussions, and all the money. I also feel close to my lab group. The members have changed over the years, but the camaraderie has stayed the same. When I joined the group there were three other graduate students and one post-doc. I worked primarily with Joe and Andrey in the ...
magnetic ordering phenomena and dynamic fluctuations in cuprate
magnetic ordering phenomena and dynamic fluctuations in cuprate

Chapter F - Totalizm
Chapter F - Totalizm

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J. J. Thomson and The Electron: 1897–1899 An Introduction

... however, is that I can use it to show students what is involved in doing science. I know of no paper that better displays the problem of marshaling evidence in the early stages of theory construction. The key experiments in this paper proceed from the working hypothesis that cathode rays consist of ...
Electronic structure of quantum dots
Electronic structure of quantum dots

The Plasma Magnet - NASA`s Institute for Advanced Concepts
The Plasma Magnet - NASA`s Institute for Advanced Concepts

... a Newton of more of thrust (or a megawatt of thrust power) is desired. The main difficulty with this approach to capturing the solar wind is the inflation of the relatively minuscule dipole field. The conditions required for inflation can be readily derived [8], but it can be seen that the magnetosp ...
Reversible Logic Synthesis with Cascades of New Gate Family
Reversible Logic Synthesis with Cascades of New Gate Family

... far from minimum and have no relation to quantum realization. Since 2001 Al-Rabadi et al proposed Galois Field approach to quantum logic synthesis (see [3-6, 34]). In this work Galois quantum matrices were proposed for swap and Toffoli gates, but without the proof that they can be built from only 1* ...
Spin-Orbit Coupling in Free-Radical Reactions
Spin-Orbit Coupling in Free-Radical Reactions

... some transitory charge movement occurs. This movement of charge can be interpreted as the source of a "transition" orbital momentum and has analogy to an atom, where despite the absence of a permanent dipole momentum, electronic dipole transitions may occur between states of different parity as the ...
Matlab Experiments Manual for
Matlab Experiments Manual for

Local Nuclear Magnetic Resonance Spectroscopy with Giant
Local Nuclear Magnetic Resonance Spectroscopy with Giant

Quantum Physics (UCSD Physics 130)
Quantum Physics (UCSD Physics 130)

Sample pages 2 PDF
Sample pages 2 PDF

Kondo Effect in Mesoscopic Quantum Dots
Kondo Effect in Mesoscopic Quantum Dots

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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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