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Revisiting quantum optics with surface plasmons
Revisiting quantum optics with surface plasmons

Lecture 19 - UConn Physics
Lecture 19 - UConn Physics

... An instrument based on induced emf has been used to measure projectile speeds up to 6 km/s. A small magnet is imbedded in the projectile, as shown in Figure below. The projectile passes through two coils separated by a distance d. As the projectile passes through each coil a pulse of emf is induced ...
Lecture 19 - UConn Physics
Lecture 19 - UConn Physics

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... MC Compared with the electric force, the gravitational force between two protons is (a) about the same, (b) somewhat larger, (c) very much larger, (d) very much smaller. (d) CQ The Earth attracts us by its gravitational force, but we have seen that the electric force is much greater than the gravita ...
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... Pulling a coil from a magnetic field. A square coil of wire with side 5.00cm contains 100 loops and is positioned perpendicular to a uniform 0.600-T magnetic field. It is quickly and uniformly pulled from the field (moving perpendicular to B) to a region where B drops abruptly to zero. At t=0, the r ...
PH2200 Exam I Spring 2004
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toolkit - The Open University
toolkit - The Open University

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NOTES AP2 Electric Potential
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C. 1
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... FMR linewidth as well as the asymmetric line shape. Such a double resonance feature can also be clearly observed in Figure 4, particularly at a high applied electric field. The appearance of the first-order standing spin wave testifies to the fact that there is a free boundary condition on one of th ...
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Phy102 L_EquiPotential

... Looking at the pattern of lines drawn, come up with some general descriptive statements about the shape of these equipotential lines. Imagine that you have a positive test charge on the positive electrode. Along what kinds of paths would this test charge travel if it were attracted along the shortes ...
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any
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LECTURE 8
LECTURE 8

< 1 ... 398 399 400 401 402 403 404 405 406 ... 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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