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Finite-Difference Time-Domain Simulation of the Maxwell
Finite-Difference Time-Domain Simulation of the Maxwell

n X ab E - Firefly
n X ab E - Firefly

... The Earth has an electric charge. The electric field strength outside the Earth varies in the same way as if this charge were concentrated at the centre of the Earth. The axes in the diagram below represent the electric field strength E and the distance from the centre of the Earth r. The electric f ...
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The Correct Derivation of Magnetism from Electrostatics

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Chapter 25.doc

... running from the origin to y = 80.0 cm, carrying the same amount of charge with the same uniform density. At the same point P , is the electric potential created by the pair of filaments (a) greater than 200 V, (b) 200 V, (c) 100 V, (d) between 0 and 200 V, or (e) 0? 14. In different experimental tr ...
Electromagnetic fields and radiation in Antennas ()
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... latter moves in the opposite direction compared to the positive charge. After a while, the current will create a magnetic field H1 that is perpendicular to the flow direction. There can’t be any electric field in the beginning because the two charges reset each other. The added current has a start v ...
Excitation of high angular momentum Rydberg states
Excitation of high angular momentum Rydberg states

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Chapter 5: Electromagnetic Forces

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Measurements of the Geometric Phase of First-Order Optical Gaussian Beams

... Geometric phase is ubiquitous in systems that undergo cyclic transformations in either parameter or state space. Manifestations of this phase have been found in many physical systems. In optics, geometric phase has had an important effect, enhancing the way optical systems are analyzed, and stimulat ...
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(positive) charge flows into the battery via the negative terminal and

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Pulse shaping control of spatially aligned

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Phases in noncommutative quantum mechanics on (pseudo) sphere

... Noncommutative quantum field theories have been studied intensively during the last several years owing to their relationship with M-theory compactifications [1], string theory in nontrivial backgrounds [2] and quantum Hall effect [3] (see e.g. [4] for a recent review). At low energies the one-parti ...
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Question paper - Unit G495/01 - Field and particle pictures
Question paper - Unit G495/01 - Field and particle pictures

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Chap. 16 Conceptual Modules Giancoli

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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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