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Optical and magneto-optical properties of UPtGe
Optical and magneto-optical properties of UPtGe

Electrostatics
Electrostatics

Class Notes #2
Class Notes #2

Slide 1
Slide 1

... over tens of gigahertz. This large frequency range opens up the possibility of probing dynamics on a nanosecond timescale. In addition, we show large rotations of up to 15π rad for continuous-wave light. Optical pulse propagation in a slow-light medium. Pulse form at various temperatures for a pulse ...
1986E1. Three point charges produce the electric equipotential lines
1986E1. Three point charges produce the electric equipotential lines

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... Potential energy is zero when magnetic dipole moment is perpendicular to the field torque tries to align magnetic dipole moment and magnetic field Derived equations are also true for any type of plane loop and not only for rectangular loops PHYS272 - Spring 17 - von Doetinchem – II/58 ...
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...detail

... galvanometer current by Thevenin’s Theorem in an unbalanced Wheatstone bridge excited by ideal voltage source; techniques of measurement of resistances including the use of Calendar and Griffith bridge and Kelvin’s double bridge; Potentiometer principle. ...
A − X Band of OH H. Christian Schewe, Dongdong Zhang,
A − X Band of OH H. Christian Schewe, Dongdong Zhang,

... no longer a good quantum number. The projection MF on the direction of Estat remains a good quantum number. Stark interference cannot be observed, however, when only an external electric field is present. The reason is that the electric field breaks parity, but does not break timereversal symmetry. ...
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2 - web.pdx.edu

The difference of the magnetic fields created by currents in neutral
The difference of the magnetic fields created by currents in neutral

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Mechanics 1: Work, Power and Kinetic Energy

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Copyright The McGraw-Hill Companies, Inc

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Theory of longitudinal magnetoresistance in weak magnetic fields

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PHYSICS Sc. (Main) B.

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Magnetism - Stevens Institute of Technology

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Chapter 17: Fields and Forces

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Experiment 1: Equipotential Lines and Electric

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1 From Last Time… Properties of electric charge Quick Quiz

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Oops !Power Point File of Physics 2D lecture for Today should have

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SEE 2053 Teknologi Elektrik - ENCON

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Realization of one-way electromagnetic modes at the interface between two

... waveguides are of particular interest in this regard. In such waveguides, there is a frequency range where waves propagate in one direction only and cannot be scattered into the reverse direction. The earliest proposals for the realization of electromagnetic one-way waveguides were presented in Refs ...
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Motivation and Objectives

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Alternating Current and Inductance.

< 1 ... 437 438 439 440 441 442 443 444 445 ... 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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