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Physics 452 - BYU Physics and Astronomy
Physics 452 - BYU Physics and Astronomy

Kinetics of decay of metastable gas phase of polarized atomic
Kinetics of decay of metastable gas phase of polarized atomic

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Dephasing and the Orthogonality Catastrophe in Tunneling through a Quantum... The “Which Path?” Interferometer

... The interference between different trajectories of a particle is one of the central postulates of quantum mechanics. The transition between classical and quantum behavior depends on when and whether this interference is realized. With the advent of mesoscopic conducting structures, it has become pos ...
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Wael`s quantum brain - Electrical & Computer Engineering
Wael`s quantum brain - Electrical & Computer Engineering

... Quantum computers also utilize another aspect of quantum mechanics known as entanglement. One problem with the idea of quantum computers is that if you try to look at the subatomic particles, you could bump them, and thereby change their value. But in quantum physics, if you apply an outside force t ...
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Physics chapter 1 electric charges and fields exercise

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A conducting circular disk has a uniform positive surface

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How to implement an application H ˚ 157

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... provide more energy to the system and would make switching more easy and would not retard the switching at all, indicating that the retardation noted for the case of charging may be solely intrinsic in nature. This observation indicates that a wholly thermodynamic approach with purely intrinsic dist ...
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Changing magnetic fields - Interactive Learning Toolkit

Slide presentation from lecture
Slide presentation from lecture

< 1 ... 108 109 110 111 112 113 114 115 116 ... 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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