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Ion Cyclotron Resonance Accelerator
Ion Cyclotron Resonance Accelerator

... worst-case field enhancement leads to a peak field of <380 kV/cm, which is well below the Kilpatrick criterion for this frequency regime [8]. Gun-to-target particle tracking was performed as explained for the one MeV ICRA. Assuming an initial phase space of 2 π mm-mrad and beam current of 2 mA, simu ...
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ppt - Harvard Condensed Matter Theory group

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PHYS 110A - HW #7

... must exist an additional bound surface charge at the position ~r = 0. We can explain this as a consequence of the point-like nature of the charge q at the center. It attracts a −q charge buildup near it, but since it has no dimensions (the definition of “pointlike”) there is no real surface to sprea ...
fermi dirac statistics in solids
fermi dirac statistics in solids

Document
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... If the medium is dispersive, equation (7.7) no longer holds. The wave changes shape as it propagates. We now consider an electromagnetic plane wave of frequency ω and wave vector and require that it satisfy not only the Helmholtz wave equation (7.3) but also all the Maxwell equations. With the conv ...
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Primer on topological insulators

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Lecture XV

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new connections between quantum and classical equations

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3.14. The model of Haldane on a honeycomb lattice

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Electric Fields - Norwell Public Schools

... • When you are close to the charge (R is small) the E-field lines are close together (indicating a stronger field ⇒ stronger Force) • As you get farther away from the charge, the lines spread out (weaker field ⇒ weaker Force) > This is why the Force is stronger when charges are closer together; the ...
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The relation of colour charge to electric charge (E/c) −P2 −Q2 −(mc

... be factored into two linear parts using 4x4 Dirac matrices. [Dirac, P.A.M., The Principles of Quantum Mechanics, 4th edition (Oxford University Press) ISBN 0-19-852011-5] This can also be done using 2x2 Pauli matrices (labelled K,L,M) because two inertial observers agree on the component of momentum ...
Energy and Momentum Considerations in an Ideal Solenoid
Energy and Momentum Considerations in an Ideal Solenoid

... T, after which the current reaches its final value. Our results showed that during that period, the electromagnetic linear momentum density is exactly balanced by the hidden momentum density. In other words, the electromagnetic force density is exactly balanced be the hidden force density. This keep ...
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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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