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Phase diagram of ultrathin ferromagnetic films with perpendicular
Phase diagram of ultrathin ferromagnetic films with perpendicular

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... magnetic field) electric field generation, which results in electron acceleration. This new effect takes place when an Alfvén wave moves along the field in the plasma which has transverse density inhomogeneity. The progressive distortion of the Alfvén wave front due to differences of local Alfvén sp ...
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Resource Doc File - Dayton Regional Stem Center

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... homodyne detection on already prepared non-Gaussian states [51, 52], see Fig. 1e. The application of these operations are not limited to single mode light fields. By using phase-space displacement or non-local photon subtraction or addition on various initial two-mode states, different kinds of enta ...
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Introduction to the AC/DC Module

< 1 ... 67 68 69 70 71 72 73 74 75 ... 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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