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Introduction to the AC/DC Module
Introduction to the AC/DC Module

Helimagnetic structure of YMn2 observed by means of nuclear
Helimagnetic structure of YMn2 observed by means of nuclear

Zahn, M., Transient Drift Dominated Conduction In Dielectrics, IEEE Transactions on Electrical Insulation EI-12, 176-190, 1977
Zahn, M., Transient Drift Dominated Conduction In Dielectrics, IEEE Transactions on Electrical Insulation EI-12, 176-190, 1977

A Wood C Ceramic D N/etal ( ) A Aluminium B Copper C Gold ( )
A Wood C Ceramic D N/etal ( ) A Aluminium B Copper C Gold ( )

Topics: • Electric Potential of continuous charge distributions
Topics: • Electric Potential of continuous charge distributions

Point Charge Dynamics Near a Grounded Conducting Plane
Point Charge Dynamics Near a Grounded Conducting Plane

IOSR Journal of Applied Physics (IOSR-JAP) ISSN: 2278-4861.
IOSR Journal of Applied Physics (IOSR-JAP) ISSN: 2278-4861.

... Fluxgate sensor can measure DC and AC magnetic fields in the range 100pT – 1mT. Fluxgate sensor has a very high sensitivity, small size, small power requirements, and has high temperature stability [14]. The sensitivity of the fluxgate sensor depends on the number of sensor windings and permeability ...
Introduction to Quantum Fields in Curved Spacetime
Introduction to Quantum Fields in Curved Spacetime

Section 24
Section 24

... x = 0, y = –d. As the moving charge passes the stationary charge, its x component of velocity does not change appreciably, but it acquires a small velocity in the y direction. Determine the angle through which the moving charge is deflected. Suggestion: The integral you encounter in determining vy c ...
HKDSE Physics Notes Waves Mechanics Mechanics Electricity
HKDSE Physics Notes Waves Mechanics Mechanics Electricity

... (d) Ways to increase the rate of evaporation (i) increase temperature of the liquid (ii) increase the surface area of the liquid (iii) decrease the humidity of air (iv) increase the movement of air Example 5 A person is wearing a wet shirt. There is 0.1 kg of water on the shirt in total. (a) How muc ...
Fulltext PDF
Fulltext PDF

Octonion model of dark matter
Octonion model of dark matter

Polarizability of a dielectric hemisphere
Polarizability of a dielectric hemisphere

Commun. Math. Phys. 110, 33-49
Commun. Math. Phys. 110, 33-49

... latter, when averaged over Φ2, is an integer for geometric reasons that were mentioned above. The two charge transports differ by two terms. The first is a tunneling term, and so, small by an application of an adiabatic theorem. The second term is not related to tunneling in any obvious way. Moreove ...
Seminar Report
Seminar Report

Agglomeration Kernel of Bipolar Charged Particles in the Presence
Agglomeration Kernel of Bipolar Charged Particles in the Presence

what sets the initial rotation rates of massive stars?
what sets the initial rotation rates of massive stars?

... presence of magnetic fields in massive stars is that they are fossil fields that were either accumulated or generated during star formation (Walder et al. 2011). Alecian et al. (2008) discovered two very young B stars with strong surface magnetic fields. They found that the younger of the two is a r ...
Nuts and Bolts of the Ion Band State Theory
Nuts and Bolts of the Ion Band State Theory

... phonons because they are expected to induce forms of coupling that directly and indirectly affect electrical (and ionic) conduction and are omitted from conventional phonon theory. These long-range forms of coupling are expected to occur because since electronic states near Ef in a PdH or PdD host h ...
PDF copy - Mechanical and Aerospace Engineering
PDF copy - Mechanical and Aerospace Engineering

Coulomb-Blockade Oscillations in Semiconductor Nanostructures
Coulomb-Blockade Oscillations in Semiconductor Nanostructures

... oscillations which they observed were due to the formation of a charge density wave or "Wigner crystal". They inferred from a model due to Larkin and Lee [22], and Lee and Rice [23], that the conductance would be thermally activated because of the pinning of the charge density wave by impurities in ...
Ch23 ISM - Siva Kodali
Ch23 ISM - Siva Kodali

... charge +Q is at the left. Near the two charges the equipotential surfaces are spheres, and the field lines are normal to the metal sphere at the sphere’s surface. Very far from both charges, the equipotential surfaces and field lines approach those of a point charge 2Q located at the midpoint. ...
FDTD MEASUREMENT OF THE REFLECTION
FDTD MEASUREMENT OF THE REFLECTION

... For simplicity, in many cases, the material parameters of the medium are approximated as constants. However, in reality, all materials, by their nature, have some form of frequency dependence of their permittivity and conductivity [3]. Therefore, the electromagnetic wave interaction with dispersive ...
Collisionless driven reconnection in an open system Ritoku Horiuchi , Wenbing Pei
Collisionless driven reconnection in an open system Ritoku Horiuchi , Wenbing Pei

Fermi Surfaces and Metals
Fermi Surfaces and Metals

Spin Conductivity in Two-Dimensional Non
Spin Conductivity in Two-Dimensional Non

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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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