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Atomic Structure
Atomic Structure

6. INTERACTION OF LIGHT AND MATTER 6.1. Introduction
6. INTERACTION OF LIGHT AND MATTER 6.1. Introduction

... One of the most important topics in time-dependent quantum mechanics is the description of spectroscopy, which refers to the study of matter through its interaction with electromagnetic radiation. Classically, light–matter interactions are a result of an oscillating electromagnetic field resonantly ...
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... (a) What is the electric field intensity at that point? (6.0 N/C [right]) (b) What force would be exerted on a charge of -7.2 x 10-4 C located at the same point, in place of the test charge? (4.3 x 10-3 N [left]) 7. What is the magnitude and direction of the electric field 1.5 m to the right of a po ...
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... induction. If the circuit is moved toward or away from the magnet or the magnet moves toward or away from the circuit, a current is induced. The magnitude of the induced emf depends on the velocity with which the wire is moved through the magnetic field, the length of the wire, and the strength of t ...
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... While this motion does create magnetic fields, over a scale much larger than an individual atom, it will average out to zero since different atoms will have their electrons circulating in different directions. 2) Spin: electrons have an intrinsic spin; this motion will create magnetic fields also. O ...
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... much more pronounced in semiconductors than in metals. Thus the voltage reading across the device can be calibrated to give the magnetic field strength directly in case the current glowing through the conducting slab is known. Hall-effective transducers can be built to be sensitive enough to detect ...
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Exercise 5 Solution

< 1 ... 592 593 594 595 596 597 598 599 600 ... 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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