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Quantum computing with nanoscale infrastructure
Quantum computing with nanoscale infrastructure

Quantum Phase Transitions - Subir Sachdev
Quantum Phase Transitions - Subir Sachdev

The origins of electrical resistivity in magnetic reconnection:
The origins of electrical resistivity in magnetic reconnection:

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... electron spins include possibilities of practical applications. Systems based on ferromagnets are very important for data storage and retrieval-magnetic memory devices including hard discs and magnetic random access memories GMR read heads. Reversal of magnetic domains is currently accomplished by a ...
Here - Lorentz Center
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... 21.5 Electric Generators A generator is the opposite of a motor – it transforms mechanical energy into electrical energy. This is an ac generator: The axle is rotated by an external force such as falling water or steam. The brushes are in constant electrical contact with the slip rings. ...
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TOPIC 19 Electric Field

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The origin of the phase in the interference of Bose

... equal to the square root of the condensate density and a phase. The state in which 具␺ˆ 共r兲典 is nonzero cannot have a fixed particle number. With one of these wave functions for each condensate, it is straightforward to discuss interference of the two, because each one has its own phase, and an inter ...
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SOLID-STATE PHYSICS II 2008 O. Entin-Wohlman

... is formed a ‘layer’ around x = 0, which is called the ‘depletion layer’, where the electron and hole concentration depends on x. In order to determine the properties of the depletion layer, we can view the abrupt change in the impurity concentration, as described by Eq. (2.1), as causing some electr ...
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TODAY Finish Ch. 20 on Sound Start Ch. 22 on Electrostatics

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Insertion Devices Lecture 2 Wigglers and Undulators

Multiphoton adiabatic rapid passage: classical transition induced by separatrix crossing
Multiphoton adiabatic rapid passage: classical transition induced by separatrix crossing

... In this paper, we present the results of fully quantum calculations for this system. We numerically solve the time-dependent Schrödinger equation for a one-dimensional model and for a full three-dimensional calculation for Li using a model potential that gives the correct quantum defects of the Ryd ...
Untitled
Untitled

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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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