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Chapter 27 Electromagnetic Induction
Chapter 27 Electromagnetic Induction

chemical potential dependence of particle ratios within a
chemical potential dependence of particle ratios within a

Ion heating resulting from pickup in magnetic reconnection exhausts
Ion heating resulting from pickup in magnetic reconnection exhausts

Solar flares
Solar flares

... Accelerating coronal charged particles requires electric fields. There are three mechanisms most often discussed in the context of acceleration of solar flare particles •DC field acceleration - E large-scale and organised •Stochastic resonant acceleration – E small-scale and random •Diffusive Shock ...
PhYSiCS
PhYSiCS

Quantum Parallelism (The Abstract of a Tutorial)
Quantum Parallelism (The Abstract of a Tutorial)

... space needed. The major difficulty in exploiting quantum parallelism lies in the fact that access to the results of a quantum computation is restricted because measurements disturb the quantum state, a process known as decoherence. Eavesdropping on a quantum communication channel can be detected wit ...
Article PDF - IOPscience
Article PDF - IOPscience

9. Orbits in stationary Potentials We have seen how to calculate
9. Orbits in stationary Potentials We have seen how to calculate

Advanced Permanent Magnetic Materials
Advanced Permanent Magnetic Materials

Quantum Chaos
Quantum Chaos

Classical limit for quantum mechanical energy eigenfunctions
Classical limit for quantum mechanical energy eigenfunctions

coulomb energy of a solitary dust grain in dusty plasma
coulomb energy of a solitary dust grain in dusty plasma

Loop Quantum Gravity and Effective Matter Theories
Loop Quantum Gravity and Effective Matter Theories

Atomic Physics - Oxford Physics
Atomic Physics - Oxford Physics

Probability Current and Current Operators in Quantum Mechanics 1
Probability Current and Current Operators in Quantum Mechanics 1

... the choice of volume of normalization. This would actually be stationary state of Hamiltonian (1) in the absence of applied fields and potentials (free qm particle). It describes a particle with precisely defined momentum p = h̄k and kinetic energy E = (h̄k)2 /2m. So it should have a nonzero current ...
Perfectly Conducting Cylinder in an External, Static
Perfectly Conducting Cylinder in an External, Static

... moving, perfectly conducting wire is associated with a uniform electric field Ez = −vB0/c in the lab frame. Note that Sr (r = a) is nonzero for the case of a moving cylinder in a magnetic field, while averaging to zero over azimuth θ . A perfect conductor at rest cannot have any Poynting flux perpen ...
Gaussian surface
Gaussian surface

... streamlines or lines of force). A flux line is drawn such that it is everywhere tangent to the electric field. A quiver plot is a plot of the field lines constructed by making a grid of points. An arrow whose tail is connected to the point indicates the direction and magnitude of the field at that p ...
The Wigner function and quantum state tomography
The Wigner function and quantum state tomography

Quantum Mechanics- wave function
Quantum Mechanics- wave function

Linköping University Post Print Doping front propagation in light-emitting electrochemical cells
Linköping University Post Print Doping front propagation in light-emitting electrochemical cells

... we would expect if the process were injection limited or electron 共or hole兲 transport limited. The front propagation speed should decrease with time in a hole- or electronlimited device as the distance that the charge carrier must migrate from the metal electrode to the front increases. An injection ...
Field Plate Models Applied to Manufacturability and
Field Plate Models Applied to Manufacturability and

Entanglement in the anisotropic Heisenberg XYZ model with
Entanglement in the anisotropic Heisenberg XYZ model with

3 - CERN Indico
3 - CERN Indico

MFF 1a: Electric Charge and A Bar Magnet
MFF 1a: Electric Charge and A Bar Magnet

Effective mass of electron in monolayer graphene: Electron
Effective mass of electron in monolayer graphene: Electron

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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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