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Objective Questions
Objective Questions

... 3. Is it possible to orient a current loop in a uniform magnetic field such that the loop does not tend to rotate? Explain. 4. Explain why it is not possible to determine the charge and the mass of a charged particle separately by measuring accelerations produced by electric and magnetic forces on t ...
98, 010506 (2007)
98, 010506 (2007)

... 2  5 kHz [19], this method can be applied only through intermediate states which induce a much larger energy splitting between paired and unpaired atoms. Here we illustrate this reading out scheme using 40 K atoms, although the technique is applicable to other species as well. Suppose the atoms i ...
ARE THERE REALLY ELECTRONS? EXPERIMENT AND REALITY
ARE THERE REALLY ELECTRONS? EXPERIMENT AND REALITY

viewgraphs for PEC presentation
viewgraphs for PEC presentation

... Materials with inherently broad spectra and weak scattering - Phonon Density Of States (DOS) of small powder samples - Magnetic excitations in correlated metals - Impurity Dynamics - Dynamics in disordered systems - Multi-magnon modes in Quantum Magnets ...
Exercise [22.29] - Road to Reality forum
Exercise [22.29] - Road to Reality forum

4.1 The Concepts of Force and Mass
4.1 The Concepts of Force and Mass

Factorization Method and the Position
Factorization Method and the Position

... as well as classical systems in curved spaces [7], just to mention few ones. The very concept of a PDM system is a fundamental problem which is far from being completely understood. Many contributions have been developed over the last years in different approaches [8–19]. In the quantum mechanical re ...
Supersymmetric quantum mechanics and the Index Theorem
Supersymmetric quantum mechanics and the Index Theorem

Quantum mechanics in more than one
Quantum mechanics in more than one

... For a given a, bmax and bmin are determined uniquely — there cannot be two states with the same a but different b annihilated by L̂+ . It also follows immediately that a = bmax (bmax +!) and bmin = −bmax . Furthermore, we know that if we keep operating on |a, bmin $ with L̂+ , we generate a sequence ...
Chapter 2 Motion Along a Straight Line Position
Chapter 2 Motion Along a Straight Line Position

GRADE 12A: Physics 5
GRADE 12A: Physics 5

Long-range forces and the Ewald sum
Long-range forces and the Ewald sum

... effect of the shifted and shifted-force alterations are demonstrated on the LJ model in Illustration 2. Note that the shifted/shifted-force modifications of the potential are not normally applied in MC simulations, since energy conservation is not an issue there. Radial distribution function One mod ...
Chapter S24
Chapter S24

... • If the electric field is zero for all points on the surface, is the electric flux through the surface zero? • If the electric flux is zero, must the electric field vanish for all points on the surface? • If the electric flux is zero for a closed surface, can there be charges inside the surface? • ...
Vector Calculus
Vector Calculus

Effects of Diffusion on Free Precession in Nuclear
Effects of Diffusion on Free Precession in Nuclear

... magnetic moments. This component, with magnitude H~, is the one which rotates in phase with the precessing moments. The phase of the rotating system will be so chosen that this B~ is along the x axis. With the rf pulse applied, the net field H= AH, k'+H, i' will determine the precession of the incre ...
Manipulation of electron spin in a quantum dot D. G
Manipulation of electron spin in a quantum dot D. G

... -orbit perturbing term, implemented by polarizing a voltage gate on top of an isolated dot, can turn one of these crossings into an anticrossing by mixing states of different quantum numbers and opening a gap. Cycling the voltage in an appropriate way allows an SU(2) Berry phase to be added to the m ...
WAVEGUIDE AND COMPONENTS
WAVEGUIDE AND COMPONENTS

Spin-2 particles in gravitational fields
Spin-2 particles in gravitational fields

Particle in a box
Particle in a box

Positron and electron collisions with anti-protons in strong magnetic fields
Positron and electron collisions with anti-protons in strong magnetic fields

... Typically, these involve the impact parameter, the velocity of the projectile and the energy and phase of the cyclotron motion. Unfortunately, perturbation theory is not applicable for the H̄ experiments. To see whether the perturbative or non-perturbative collisions play the largest role, the dista ...
Chapter S24
Chapter S24

quantum field theory, effective potentials and determinants of elliptic
quantum field theory, effective potentials and determinants of elliptic

20.3 Coulomb`s Law - 20.4 The Concept of the Electric Field.notebook
20.3 Coulomb`s Law - 20.4 The Concept of the Electric Field.notebook

PPTX - University of Toronto Physics
PPTX - University of Toronto Physics

Resonant reflection at magnetic barriers in quantum wires - ITN
Resonant reflection at magnetic barriers in quantum wires - ITN

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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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