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Supersymmetric quantum mechanics and new potentials
Supersymmetric quantum mechanics and new potentials

... From the potentials studied (particle in the box, Poschl-Teller and RosenMorse) we obtained new potentials (eq. (22), (32) and (43)), which are different from the original ones, but whose spectra and eigenfunctions are known. The relation between the old system and the new one is established through ...
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... Note: If there is a changing flux, there will be an induced emf, B however, if dΦ dt = 0 there could still be emf in a wire from other effects. (Enet = EF + Eother ) ...
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... Because this current in the left-hand side of the loop is in a downward magnetic field, there will be a magnetic force to the left. To keep the rod moving, there must be an equal external force to the right, given by F  IlB . ...
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The Dot Product of Two Vectors

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Deflection of Electrons by Electric and Magnetic Fields
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... Compare your calculated and experimental deflection sensitivities. Show how the deflection sensitivity varies with the accelerating voltage. 4) Determine the deflection sensitivity due to a magnetic field produced by a current in the magnetic deflection coils. Choose a single value of the accelerati ...
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Schrödinger`s equation

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An investigation into student understanding of vectors and

< 1 ... 333 334 335 336 337 338 339 340 341 ... 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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