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Vacuum friction in rotating particles
Vacuum friction in rotating particles

Electronic structure of mixed valence transition metal oxides
Electronic structure of mixed valence transition metal oxides

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Slide 1

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... WEIGHT just like coulomb’s law is symbolic of Newton’s Law of Gravitation. The symbol for Electric Field is, “E”. And since it is defined as a force per unit charge he unit is Newtons per Coulomb, N/C. NOTE: the equations above will ONLY help you determine the MAGNITUDE of the field or force. Concep ...
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Residual Magnetic Flux Density Distribution Calculation

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... Hence, the equation for the velocity field (P) of points of the disk becomes r r r r r r r r v(P) = v(x,y,z) = ω k × (x i + y j + z k) = - ω y i + ω x j • Note that the vector function defined by the above equation can be evaluated mathematically for any point P(x,y,z) in the whole space. • However, ...
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Physics 30 - Structured Independent Learning

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Structural, electric, and magnetic properties of Mn perovskites

... the occupation of a lower level make the system more stable. This phenomenon is called the Jahn-Teller effect. [2] 3. Semicovalent Exchange Interaction The cooperative ordering of this Jahn-Teller distortion results in the corresponding magnetic, i.e. spin, order in a system from the semicovalent ex ...
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Phys. Rev. Applied 2, 024002

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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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