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Quantum path-integral study of the phase diagram and isotope
Quantum path-integral study of the phase diagram and isotope

... of neon is thus interesting because allows us to quantify systematic errors of treating the neon atoms as particles moving classically in the PES. However, we stress that these quantum corrections do not represent any kind of measurable property, i.e., they can not be directly compared to experiment ...
Thermal equilibrium states for quantum fields on
Thermal equilibrium states for quantum fields on

... yield only tiny deviations from the predictions of usual QFT. However, it is not very clear what these deviations are, or how they could be observed. In the model at hand, the effect of the noncommutativity parameter θ on scattering processes (at zero temperature) was investigated in [GL07], and sho ...
Simulation of Charged Particle Orbits in Fusion
Simulation of Charged Particle Orbits in Fusion

Physics - PCMBToday
Physics - PCMBToday

Lecture 23
Lecture 23

... relative to a nucleus. 2. ionic: comes from the displacement of a charged ion with respect to other ions. 3. dipolar: from molecules with a permanent electric dipole moment that can change orientation in an applied electric field. ...
Quantum Mechanics_chemical potential
Quantum Mechanics_chemical potential

... In recent years, thermal physics has applied the definition of chemical potential to systems in particle physics and its associated processes. For example, in aquark–gluon plasma or other QCD matter, at every point in space there is a chemical potential for photons, a chemical potential for electron ...
OpenStax Physics Text for 2B - Chapter 5
OpenStax Physics Text for 2B - Chapter 5

Chapter 16
Chapter 16

Chapter 4 Gauss’s Law
Chapter 4 Gauss’s Law

... In general, a surface S can be curved and the electric field E may vary over the surface. We shall be interested in the case where the surface is closed. A closed surface is a surface which completely encloses a volume. In order to compute the electric flux, we r divide the surface into a large numb ...
Quantum Chaos and Quantum Information
Quantum Chaos and Quantum Information

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Theoretical and experimental status of magnetic monopoles

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Return of the Ether: Conjecture That Can Explain

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22 magnetism - Wright State University

Electronic Correlations in Transport through Coupled Quantum Dots V 82, N 17
Electronic Correlations in Transport through Coupled Quantum Dots V 82, N 17

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Chapter 9: Electromagnetic Waves

AP Physics - Static Electricity
AP Physics - Static Electricity

Unusually Large Franz-Keldysh Oscillations at Ultraviolet Wavelengths in Single-Walled Carbon Nanotubes
Unusually Large Franz-Keldysh Oscillations at Ultraviolet Wavelengths in Single-Walled Carbon Nanotubes

Spin Hall Effect
Spin Hall Effect

Pair production processes and flavor in gauge
Pair production processes and flavor in gauge

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Pair production in counter-propagating laser beams

Electron Cloud Dynamics in the CesrTA Wiggler
Electron Cloud Dynamics in the CesrTA Wiggler

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(pdf)

... The collision-induced dissociation 共CID兲 of the N2 molecule by an energetic nitrogen atom is a process of importance in the upper atmosphere of Titan, a moon of Saturn, which has a nitrogen atmosphere.1 The energized nitrogen atoms produced by dissociation populate Titan’s atmospheric corona and can ...
Wiggler_dynamics_PRST-AB
Wiggler_dynamics_PRST-AB

... in x at higher |z|. To explain this pattern one must refer to the field geometry as shown in Fig. 7. Bx and the variations of the field with x are essentially negligible, so it is enough to show, as in the figure, the magnetic field lines at x=0 in the y-z plane. There are four different field line ...
CJ Electrostatics Assignment 1 Solutions
CJ Electrostatics Assignment 1 Solutions

contribution to the quantum theory of light scattering
contribution to the quantum theory of light scattering

< 1 ... 88 89 90 91 92 93 94 95 96 ... 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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