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THE EARTH`S MAGNETIC FIELD
THE EARTH`S MAGNETIC FIELD

... • The Earth’s magnetic field can be mapped by means of isomagnetic charts. These are explained on the next page. • Secular variations are slow changes in the Earth’s magnetic field with time. For example magnetic north drifts gradually over the years. • Polarity reversals: There is very strong evide ...
Voltage-tunable ferromagnetism in semimagnetic quantum dots with
Voltage-tunable ferromagnetism in semimagnetic quantum dots with

... material systems.4 This ability to externally control the properties of magnetic crystals with means other than the external magnetic field may have important device applications. An important feature of modern nanotechnology is the ability to shape semiconductor crystals, designing their quantum pr ...
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ch15 lecture-1-2-S06

... Each particle experiences the same electric force and the same acceleration. (b) The electric force on the proton is greater in magnitude than the force on the electron but in the opposite direction. (c) The electric force on the proton is equal in magnitude to the force on the electron, but in the ...
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Electromagnetic braking: A simple quantitative model - if

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vacuum particle creation in strong fields as the field induced phase
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Photon localizability - Current research interest: photon position

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Entanglement, Decoherence and the Quantum/Classical

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Plasma environment of magnetized asteroids

... To sum up the basic idea of these boundary conditions, the electromagnetic field quantities as well as the moments of the particle distribution function are fixed on constant, timeindependent values in the inner region. Of course, the divergence of the magnetic field vanishes at the grid points insi ...
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The watt-balance operation: magnetic force and induced electric

... the geometric factor BL, we obtain the equation mgu = UI, which virtually relates mechanical and electrical powers and allows m to be determined in terms of electrical quantities and, hence, of the Planck constant. A number of subtleties have been dismissed in the previous analysis. Firstly, the Lor ...
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... X, momentum P! via potential v (x,X). At the same time the heavier particle experiences an external potential V(X). The two-particle Hamiltonian consequently has the form P2 p2 ...


... bound charges. In class we discussed the physical interpretation of bound charges. The displacement of the charges in the material caused by the polarization will only result in a net charge near the surface of the material or near areas where the polarization is not constant, i.e. has a non-zero di ...
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UV practice

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Concepts of condensed matter physics Spring 2014 Exercise #5

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Academia Sinica, Taipei, Taiwan, 06/2010, Yip Sungkit

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Chapter 17 Notes

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Monopoles and fractional vortices in chiral superconductors

Resonant ionization of shallow donors in electric field Linköping University Post Print
Resonant ionization of shallow donors in electric field Linköping University Post Print

... 3.1 MV/m [cf. figure 1(a)], which will be argued to correspond to the anti-crossings at 2.45 and 3.25 MV/m observed in [4], despite of the disagreement in the critical-field values. Let us regard first the dependence of the energy of the ground state on the electric field [figure 1(a)]. This depend ...
Final Review
Final Review

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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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