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Is Classical Electrodynamics an Inconsistent Theory? - Philsci
Is Classical Electrodynamics an Inconsistent Theory? - Philsci

... Maxwell-Lorentz equations when the particle involved is an extended particle, we have to spell out how the history of such a particle is represented, how such a history determines the charge and current densities, and how one applies the Lorentz force law to such a particle. Our spherical particle i ...
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Chapter 1 Elementary solutions of the classical wave equation
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... this solution is also a solution of the Wave equation. Classically there are a number of problems with fields from point like sources. One of the more severe is that energy and momenta and spin of these fields become infinite if we do not apply some sort of cut-off at small distances. For the energy ...
FINAL EXAM
FINAL EXAM

... You are not required to answer all questions in this exam. You will receive points toward your exam points for every question correctly answered. Partial credit is available, however a minimum amount of work and explanation must be shown to receive any credit (for example, a mere list of equations w ...
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Final Paper - University of Calgary

Compton Scattering Sum Rules for Massive Vector
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Haldane charge conjecture in one-dimensional

... where δni = ni − hni i. The quantum phase transition between the SP-CDW phases is found to belong to the U(1) universality class. There is a second duality symmetry with ξL6 → −ξL6 which is a symmetry of Eq. (3) if g2,5 → −g2,5 . This duality symmetry is non-local in terms of the original lattice fe ...
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... • Therefore, the electric flux through a closed surface is the sum of the normal components of the electric field all over the surface. • The sign matters!! Pay attention to the direction of the normal component as it penetrates the surface… is it “out of” or “into” the surface? • “Out of” is “+” “i ...
Towards a Quantum Field Theory of Mind
Towards a Quantum Field Theory of Mind

... or part of an atom, is manifested for an instant. When no observation takes place, the quantum wave function “hangs around,” like a ghost, in the same locale in which it first popped. This sequence is highly reinforced by the repeating structure. Habitual observation eventually becomes so reinforced ...
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... Laplace's equations - uniqueness theorems - potential of a localised charge distribution - electric potential energy of a continuous charge distribution - multi pole expansion: approximate potentials at large distances - monopole and dipole terms - electric dipole moment - electric field of a dipole ...
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... Geomagnetic activity is influenced by the combination of a wide variety of conditions in the solar wind and magnetosphere, but the single most decisive parameter is the north-south component (B Z ) of the interplanetary magnetic field (IMF). Keeping all other parameters at average values, a small, p ...
Cloaking of Matter Waves
Cloaking of Matter Waves

... two sets of trajectories would exactly match. Using the Hamiltonian Eq. (8), it is straightforward to show that this leads to the relations mr1 =mr2  m1 =m2  m1 =m2 and V2  1  mr1 =mr2 E  mr1 =mr2 V1 . If (m^ 1 , V1 ) correspond to the perfect cloaking conditions Eq. (6), ^ 2 , V2 ) wou ...
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... Interaction of THz photons with a 2DEG in a semiconductor provides the basis for a number of different THz-detection schemes. One of the simplest approaches makes use of free carrier absorption to heat the electron gas relative to the lattice to change the conductivity. But it requires low-temperatu ...
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الشريحة 1 - جامعة فلسطين

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Simultaneous optical trapping and detection of atoms by microdisk

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Relativistic Quantum Mechanics

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The potential quark model in theory of resonances

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Phases of Matter and Phase Transitions

(DOC, Unknown) - Natural Philosophy Alliance
(DOC, Unknown) - Natural Philosophy Alliance

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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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