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Solvation of electronically excited I2-
Solvation of electronically excited I2-

IOSR Journal of Mathematics (IOSR-JM)
IOSR Journal of Mathematics (IOSR-JM)

... Considerable attention has been given to the unsteady free convection flow of viscous incompressible, electrically conducting fluid in presence of applied magnetic field in connection with the theories of fluid motion in the liquid core of the Earth and also meteorological and oceanographic applicat ...
In situ electron plasma in a Penning–Malmberg trap
In situ electron plasma in a Penning–Malmberg trap

Proton chemical shifts in NMR. Part 8.1 Electric field effects and
Proton chemical shifts in NMR. Part 8.1 Electric field effects and

... SCS but concluded that this term was not significant and ignored it subsequently. More recent investigations have only partially clarified the situation. The proton SCS of ketones, thioketones 10–12 and ethers 13 were interpreted as arising from anisotropy and electric field effects but for alcohols ...
emp10_04
emp10_04

Syllabys for BSc(Major):
Syllabys for BSc(Major):

... Unit I: Electromagnetic fields (No. of Lectures: 15) (Marks: 24) Electromagnetic induction, displacement current , Maxwell’s field equations and their interpretations (integral and differential forms), electromagnetic potentials, (scalar and vector potential) Derivation of Maxwell's wave equations, ...
Suppression of error in qubit rotations due to Bloch–Siegert oscillation... resonant Raman excitation
Suppression of error in qubit rotations due to Bloch–Siegert oscillation... resonant Raman excitation

... strong driving field, the BSO correction to the usual Rabi oscillation could be a significant fraction. For example, in a recent experiment by Martinis et al [11], the BSO amplitude was on the order of 1% of the usual Rabi oscillation. For a still stronger driving field, this amplitude could be as l ...
Pauline Oliveros and Quantum Sound
Pauline Oliveros and Quantum Sound

4 - ckw
4 - ckw

Electromigration instability: Transgranular slits  in  interconnects
Electromigration instability: Transgranular slits in interconnects

... passing per length per time), D, the surface diffusivity, I?~ the thickness of the surface layer taking part in the diffusion process, R the atomic volume, k the Boltzmann constant, T the absolute temperature, 2: (>O) the effective valence, e the magnitude of the electron charge, E, the electric fie ...
In search of symmetry lost
In search of symmetry lost

4 - ckw
4 - ckw

GDR-PH-QCD, IPNO 7/XII/2012
GDR-PH-QCD, IPNO 7/XII/2012

P3 ELECTRICITY
P3 ELECTRICITY

... As an alternative to measuring with the torsion balance, the coulomb force between two spheres can also be determined using the force sensor. This device consists of two bending elements connected in parallel with four strain gauges in a bridge configuration; their electrical resistance changes when ...
Self-Force Reduced Finite Element Poisson Solvers for Monte Carlo
Self-Force Reduced Finite Element Poisson Solvers for Monte Carlo

quantum dynamics of integrable spin chains
quantum dynamics of integrable spin chains

... The extension to local observables was done in the study of impurity models. Both Tjon [27], and Abraham, Barouch, Gallavotti and Martin-Löf [1, 2, 3] have found the same kind of behavior for the XX model with an impurity. So, definitely, this unusual behavior of such systems could be discouraging, ...
TRANSMISSION AT THE NEUROMUSCULAR
TRANSMISSION AT THE NEUROMUSCULAR

... 1. List the major events that occur in transmission at a chemical synapse. 2. List the specific events that occur at the neuromuscular junction (motor endplate). 3. State that acetylcholine is released in discrete packets called "quanta", each quantum corresponding to one presynaptic vesicle. 4. Def ...
Probing Dark Energy with Atom Interferometry.
Probing Dark Energy with Atom Interferometry.

ll ne - Arihant Book
ll ne - Arihant Book

... charge can neither be created nor be destroyed. In any physical process, the charge may get transferred from one part of the system to another, but the net charge will always remain the same. It is impossible to create or destroy net charge carried by an isolated system although charge carrying part ...
Electrostatic energy calculation for the interpretation of scanning
Electrostatic energy calculation for the interpretation of scanning

Synchronization of Spin Torque Oscillators
Synchronization of Spin Torque Oscillators

... of magnetizations having several different phase differences, depending on the material parameters, by numerically solving the Landau-Lifshitz-Gilbert (LLG) equation [28]. In this paper, the synchronization of spin torque oscillators through the spin Hall magnetoresistance effect is studied theoreti ...
Electric field of due to a point charge.
Electric field of due to a point charge.

Hyperbolic Geometrodynamic Warp Drives
Hyperbolic Geometrodynamic Warp Drives

... function a = 1/ β , but why this function is accurate gets into metaphysics. A similar phenomenon was noted in a series of experiments conducted by Antoon Hendrik Lorentz, as the acceleration rates of electrons also seemed to be strangely governed by the beta function. Thus for all intents an purpos ...
Mutual shielding of closely spaced dust particles
Mutual shielding of closely spaced dust particles

Phases of correlated spinless fermions on the honeycomb lattice
Phases of correlated spinless fermions on the honeycomb lattice

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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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