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Spin-liquids
Spin-liquids

Capacitor: any two conductors, one with charge +Q, other with
Capacitor: any two conductors, one with charge +Q, other with

BilaksPhysiks
BilaksPhysiks

... 3. What type of path will the proton follow if only the motion in the x-y plane is considered? A: Straight line (Linear) B: Parabolic C: Circular This is due to the horizontal component of the initial velocity. ...
Bose-glass and Mott-insulator phase in the disordered boson Hubbard model
Bose-glass and Mott-insulator phase in the disordered boson Hubbard model

... Fig. 5, we get firm support for z51: The ratio of the decay exponents y x and y t for C x and C 1 ( t )5 @ C 1 i ( t ) # av , respectively, should equal z and we find y x /y t '1.0(1), roughly independent of how we scale L t with L. From y x 5d1z221 h we get h50.160.1. Finally the inset of Fig. 5 sh ...
Orbits in a central force field: Bounded orbits
Orbits in a central force field: Bounded orbits

... The nature of boundedness of orbits of a particle moving in a central force field is investigated. General conditions for circular orbits and their stability are discussed. In a bounded central field orbit, a particle moves clockwise or anticlockwise, depending on its angular momentum, and at the sa ...
Cloud Chamber - Wabash College
Cloud Chamber - Wabash College

... FIG. 2. In (a), we demonstrate the actual trajectory of a positive muon decay [5] and in (b) we show the theoretical trajectory as viewed from the top down of our setup. The magnetic field produced by our apparatus is approximately uniform and points up. By the Lorentz force law, a positively charge ...
Show by a theoretical and experimental argument that potassium
Show by a theoretical and experimental argument that potassium

Electrical Potential
Electrical Potential

Non-singular field-only surface integral equations for
Non-singular field-only surface integral equations for

Physics 208
Physics 208

Direct measurement of the effective charge in nonpolar suspensions
Direct measurement of the effective charge in nonpolar suspensions

Class Notes
Class Notes

Classical Electrodynamics - Institut für Theoretische Physik
Classical Electrodynamics - Institut für Theoretische Physik

chapter26_p
chapter26_p

MATTER UNIFIED ISBN 91-973818-7-X 12
MATTER UNIFIED ISBN 91-973818-7-X 12

... constitutes of a single, charged particle, moving in a closed loop around a force centre, as for example is the case of an electron moving around the nucleus core. The Bohr “magneton” is such a case, constituting the magnetic momentum for an electron that is situated in the innermost orbit of a hydr ...
Magnetoconductivity of two-dimensional electrons on liquid helium:
Magnetoconductivity of two-dimensional electrons on liquid helium:

... Two-dimensional electrons in surface states above superfluid helium form the simplest conducting system known experimentally.1 Below 1 K the electrons are in the quantum ground state of the potential well formed by the helium surface and a vertical electric field. However, they are free to move hori ...
Probability, Expectation Values, and Uncertainties
Probability, Expectation Values, and Uncertainties

Electric Stress Estimation and Control
Electric Stress Estimation and Control

Sheath properties and related phenomena of the plasma wall
Sheath properties and related phenomena of the plasma wall

... higher fluxes of about 10 MW/m2 are estimated for the divertor in the future ITER machine. This means that Pilot-PSI can be successfully used for studying plasma-surface interaction at physical parameters that are interesting for fusion devices. 2.3 Electron Multi-Channel Analyzer The working princi ...
IOSR Journal of Mathematics (IOSR-JM)
IOSR Journal of Mathematics (IOSR-JM)

... Problems of loads moving subsonic, transonic and supersonic velocity in a half-space have been discussed among others, by Cole and Huth [4], Fung [5] and Fryba [6]. Payton[7] has considered the transient motion of an elastic half-space due to a moving line load, and also the problem of steady-state ...
Book 1
Book 1

Computation of hadronic two-point functions in Lattice QCD
Computation of hadronic two-point functions in Lattice QCD

... The masses of the hadrons are much bigger than the masses of their valence quarks. Moreover, md − mu  ms , mπ , mn . So usually the approximation mu ≈ md ≈ mud = (mu + md )/2 is employed and electromagnetic interactions are neglected. In this particular limit the socalled isospin symmetry is realiz ...
PDF only - at www.arxiv.org.
PDF only - at www.arxiv.org.

Magnetic Neutron Scattering
Magnetic Neutron Scattering

... instrumentation and theoretical modelling should be done on an absolute scale, i.e. in units of barn. It is a common practice, that experimental data is not well calibrated (in intensity) and theoretical models predictions are done in arbitrary units. To see how common this practice is, please just ...
Quantum Distinction: Quantum Distinctiones!
Quantum Distinction: Quantum Distinctiones!

< 1 ... 164 165 166 167 168 169 170 171 172 ... 661 >

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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