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Faraday`s Experiment
Faraday`s Experiment

b - FIU
b - FIU

... •  If we chose Ub=0, then U(y)=q0Ey •  V(y)=U(y)=Ey=? •  What if Ub is not 0? What is Ua-Ub? Va-Vb? ...
one mark | physics english medium
one mark | physics english medium

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High-field miniband transport in semiconductor superlattices in

... dence of the current it has been concluded that acousticphonon-assisted ~quasielastic! scattering is not dominant.8 Combined Stark-cyclotron resonances have also been identified in photocurrent measurements.11 As the magnetic field was increased, the intensity of the Stark transitions was enhanced a ...
PHYS 632 Lecture 10: Induction
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... The shock waves employed were in the Mach number range 10 to 12 in a 2 / 3 Ar-1 / 3 H2 mixture (by volume) and produced temperatures of the order of 4600°K at densities high enough to ensure thermal equilibrium. Under these conditions there was negligible ionization or excitation of the argon diluen ...
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Homework #3 consists of only one part as follows:

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Chapter 6 OPTICAL PROPERTIES OF SOLIDS We will investigate

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Lecture 16a_Electromagnetic 1

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... There is a notable difference in the spectra of (highly non-relativistic) cyclotron radiation and (highly relativistic) synchrotron radiation. The cyclotron radiation is all emitted at the cyclotron frequency ωcyc = eB/me c. The synchrotron radiation is emitted over a broad range of frequencies up t ...
From last time… Today: Electromagnetic waves, electricity and
From last time… Today: Electromagnetic waves, electricity and

... Fri. Feb 17, 2006 ...
File
File

File
File

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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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