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nunn_dungey_paper_v2 - Electronics and Computer Science
nunn_dungey_paper_v2 - Electronics and Computer Science

... resonance velocity in the frame of the resonant particle, such as might be due to a gradient of wave number k for example. In the second term F represents an external DC force such as might be due to a DC electric field or more realistically the mirror force in a magnetic field dipole geometry. It w ...
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3. Derivation of the two-dimensional ideal dipole model

... Rationalizing (S4.6) yields:  2 Ib  h2  2h cos  1   2 I1h  b2  2b cos  1  1I 2b  h2  2h cos  1. ...
Quantum nature of laser light
Quantum nature of laser light

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... only while an external field is being applied. It is induced by a change in the orbital motion of electrons due to an applied magnetic field. The magnitude of the induced magnetic moment is extremely small, and in a direction opposite to that of the applied field (Fig. 20.5a). - r < 1, m ( -10-5) ...
Magnetic Pulsations: Sources and Properties
Magnetic Pulsations: Sources and Properties

attosecond light pulses
attosecond light pulses

... single frequency. Only the intensity dependent, nonlinear part of the index of refraction of the Sapphire crystal enables a cavity design that locks all the frequencies over the full gain bandwidth of the Ti:Sa medium to yield a single femtosecond pulse that roundtrips in the cavity. Every time the ...
CHAPTER 2 THE ELECTRIC STRUCTURE OF THE
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Capacitance - Engineering Sciences
Capacitance - Engineering Sciences

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Ultrahigh magnetic fields produced in a gas .. puff Z pinch

... or initial magnetic field is created by a Helmholtz coil. A schematic illustration of a gas-puff Z pinch with a frozen-in axial magnetic field is shown in Fig. 1. The nozzle for the gas puff ejects a gas into the region between the cathode and the anode, and the axial field coils produce an axial ma ...
Final exam - Department of Physics and Astronomy : University of
Final exam - Department of Physics and Astronomy : University of

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EXAMPLE 6 Find the gradient vector field of . Plot the gradient vector

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USING STANDARD SYSTE - The University of Iowa

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Lab 7: Faraday Effect and Lenz` law Physics 208

... fields, produced by permanent magnets and by loops of current. These static fields varied throughout space in direction and magnitude, but were the same at all times. This week you discover some very unusual properties of time-varying magnetic fields. In particular, a time-varying magnetic field pro ...
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Electric charges of the same sign

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... vibrates with both ends fixed. However, with wind instruments (trumpet, trombone, etc.), we can have the situation where both ends are free and a different situation where one end is free and one end is fixed. 1. If both ends are free, we get the same resonance condition as for both ends fixed: #(/ ...
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Modification of Electric and Magnetic Fields by Materials

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Oscillating dipole model for the X-ray standing wave enhanced

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Iron nail` Iron nail` Iron nau`

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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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