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Waxman
Waxman

Quantum Monte Carlo study of a disordered 2D Josephson junction array
Quantum Monte Carlo study of a disordered 2D Josephson junction array

... at temperature T ¼ 0. The reason is that there is a second energy which becomes important in small grains, namely the charging energy of the grains [5]. The crucial physics is then determined by the competition between this charging energy and the Josephson coupling energy. If the charging energy is ...
Phys. Rev. A 62, 062304
Phys. Rev. A 62, 062304

non equilibrium dynamics of quantum ising chains in the presence
non equilibrium dynamics of quantum ising chains in the presence

Iron nail` Iron nail` Iron nau`
Iron nail` Iron nail` Iron nau`

Three-dimensional electron magnetohydrodynamic reconnection. I
Three-dimensional electron magnetohydrodynamic reconnection. I

Quantum Hall ferromagnet at high filling factors: A magnetic
Quantum Hall ferromagnet at high filling factors: A magnetic

Physics 12 Class th
Physics 12 Class th

Whistler oscillitons revisited: the role of charge neutrality?
Whistler oscillitons revisited: the role of charge neutrality?

... arises between the weakly nonlinear results obtained from the derivative nonlinear Schrödinger equation, predicting envelope solitons (where the amplitude is stationary in the wave frame, but the phase is not), and recent results for whistler oscillitons, indicating that really stationary structure ...
16.9 Electric Fields and Conductors
16.9 Electric Fields and Conductors

Topological insulators
Topological insulators

Module P4.4 Electromagnetic induction
Module P4.4 Electromagnetic induction

... circuit. ☞ There will only be an induced current in response to the induced voltage if there is a complete circuit through which the current can flow1— 1but the induced voltage can exist even when the meter circuit is incomplete and there is no an induced current. In this sense, the induced voltage ...
Chapter 2 Motion of Charged Particles in Fields
Chapter 2 Motion of Charged Particles in Fields

... Figure 2.18: Suddenly turning on an electric field causes a shift of the gyrocenter in the direction of force. This is the polarization drift. Start­up effect: When we ‘switch on’ an electric field the average position (gyro center) of an initially stationary particle shifts over by ∼ 12 the orbit size ...
Transmitted and reflected electrons and the collisionless shock front
Transmitted and reflected electrons and the collisionless shock front

... Electron heating and acceleration are the central problems of astrophysical shock physics since shock energized electrons are believed to be responsible for the electromagnetic emission from supernova remnants, gamma ray bursts, relativistic jets and others. This emission is the only evidence of the ...
Art Hobson There are no particles, there are only fields 1
Art Hobson There are no particles, there are only fields 1

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Slides - Agenda

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Force and Current Powerpoint

... field so when it crosses through zero it will ...
Induction and Inductancesv
Induction and Inductancesv

Electric and magnetic dipole allowed transitions of atoms for three
Electric and magnetic dipole allowed transitions of atoms for three

Contents Syllabus
Contents Syllabus

... FARADAY’S LAWS OF ELECTROMAGNETIC INDUCTION : (i) When magnetic flux passing through a loop changes with time or magnetic lines of force are cut by a conducting wire then an emf is produced in the loop or in that wire. This emf is called induced emf. If the circuit is closed then the current will be ...
Computing with Atoms and Molecules
Computing with Atoms and Molecules

Recurrence spectroscopy of atoms in electric fields: Scattering in the...
Recurrence spectroscopy of atoms in electric fields: Scattering in the...

Solar wind electron interaction with the dayside lunar surface and... magnetic fields: Evidence for precursor effects
Solar wind electron interaction with the dayside lunar surface and... magnetic fields: Evidence for precursor effects

... with reflection by a downward parallel electric field. The second type of event, with an apparent upward-going conic (58% of observations), has a similar loss cone to the first, but with enhanced flux surrounding this loss cone. The flux enhancement consists of “wings” on the upwardgoing half of the ...
Problem I Problem II - Physics Department, Princeton University
Problem I Problem II - Physics Department, Princeton University

Quantum Optics - Assets - Cambridge University Press
Quantum Optics - Assets - Cambridge University Press

... many of the ideas with typical applications. We make every possible attempt to indicate the experimental work if an idea has already been tested. Other applications are left as exercises which contain enough guidance so that the reader can easily work them out. Important references are given, althou ...
< 1 ... 122 123 124 125 126 127 128 129 130 ... 661 >

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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