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Quantum annealing with manufactured spins
Quantum annealing with manufactured spins

b) a - Purdue Physics
b) a - Purdue Physics

The control of the viscosity of a suspension by the application
The control of the viscosity of a suspension by the application

the hydrogen atom in a uniform magnetic field - an example
the hydrogen atom in a uniform magnetic field - an example

Partial focusing of radiation by a slab of indefinite
Partial focusing of radiation by a slab of indefinite

... however, are not fixed, but rather vary with the direction of propagation in the material with respect to the principal axes. The condition that the wave vector parallel to the interface be conserved implies two possible solutions in the medium, which can be distinguished by requiring the group velo ...
Derivation of Fresnel Equations
Derivation of Fresnel Equations

... The intensity of light reflected from the surface of a dielectric, as a function of the angle of incidence was first obtained by Fresnel in 1827. When an electromagnetic wave strikes the surface of a dielectric, both reflected and refracted waves are generally produced. The reflected wave has a dire ...
Phase control of trapped ion quantum gates
Phase control of trapped ion quantum gates

... quantum control, interferometry (Some figures in this article are in colour only in the electronic version) Scalable quantum computing presents a direct application for the study and control of large-scale quantum systems. The generally accepted requirements for quantum hardware [1] include identifi ...
Jeopardy EM Waves and Magnetism
Jeopardy EM Waves and Magnetism

a) clockwise b) counterclockwise c) no induced
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Assessing the Nonequilibrium Thermodynamics in a
Assessing the Nonequilibrium Thermodynamics in a

... implications for the statistics of work coming from considering processes described by operators that either commute or do not commute with the unperturbed Hamiltonian of a given system. We consider a quantum many-body system and derive an expression that allows us to give a physical interpretation, ...
Magnetoconvection in HCLL Blankets
Magnetoconvection in HCLL Blankets

Duality Theory of Weak Interaction
Duality Theory of Weak Interaction

1 - web page for staff
1 - web page for staff

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Mixed quantum–classical dynamics
Mixed quantum–classical dynamics

Magnetic fields of charged particles in motion
Magnetic fields of charged particles in motion

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A Functional Architecture for Scalable Quantum Computing
A Functional Architecture for Scalable Quantum Computing

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AP Physics B Lesson Plans

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Lecture 2 - Purdue Physics

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are quantum physics and spirituality related?
are quantum physics and spirituality related?

... energy, and about kinetic energy: kinetic energy is energy to do with motion, and potential energy is to do with what would happen if the circumstances were right. In classical physics we can go a long way by knowing about conservation of energy (as well as conservation of momentum, angular momentum ...
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Negative refractive index metamaterials - Dimitri Basov

... increasingly routine, the prospect of designer materials with a range of new and selectable EM properties at nearly any wavelength band is nearing reality. By providing access to new realms of material response, MMs have and will continue to impact the fields of physics, materials science, engineeri ...
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Subauroral morning proton spots (SAMPS) as a result of

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Document

PERFORMANCE ANALYSIS OF POINT SOURCE MODEL WITH
PERFORMANCE ANALYSIS OF POINT SOURCE MODEL WITH

CNTMOSFETsrev5 - University of Maryland
CNTMOSFETsrev5 - University of Maryland

< 1 ... 102 103 104 105 106 107 108 109 110 ... 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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