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Quadratic response theory for spin-orbit coupling in semiconductor
Quadratic response theory for spin-orbit coupling in semiconductor

124. Franzen S. “Intrinsic Limitations on the |E|4 Enhancement
124. Franzen S. “Intrinsic Limitations on the |E|4 Enhancement

... reported enhancement factors have continued to increase as new nanoparticle geometries were investigated.14-17 Since single molecule Raman scattering on a single particle14,18 is difficult to explain theoretically,19-22 there is a growing consensus that large SERS enhancement requires more than one ...
Electricity and Magnetism - U
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QUANTUM COMPUTING

Decoherence and the Transition from Quantum to Classical
Decoherence and the Transition from Quantum to Classical

... If macroscopic systems cannot be always safely placed on the classical side of the boundary, then might there be no boundary at all? The Many Worlds Interpretation (or more accurately, the Many Universes Interpretation), developed by Hugh Everett III with encouragement from John Archibald Wheeler in ...
Projections and correlations in the fractional quantum Hall effect
Projections and correlations in the fractional quantum Hall effect

Electric current and magnetic field geometry in flapping magnetotail
Electric current and magnetic field geometry in flapping magnetotail

... 0 ∇×B calculated from four-point magnetic field measurements was the largest component during both crossings, and showed a bipolar variation: jz >0 during the first crossing and jz <0 during the second one. This indicates a strong tilt of the current sheet in the Y −Z plane. During the first crossin ...
The Haldane-charge conjecture
The Haldane-charge conjecture

geometric phases in quantum theory
geometric phases in quantum theory

... reach the equator and then move it parallel along the equator till another meridian which keeps an angle of θ with the original one. Then you move the vector back to the north pole along the new meridian again keeping it always parallel. When you reach the north pole you discover that the vector poi ...
Superconducting Qubits and the Physics of Josephson Junctions
Superconducting Qubits and the Physics of Josephson Junctions

A study of the electron structure of endohedrally confined atoms
A study of the electron structure of endohedrally confined atoms

Charge, spin and orbital order in the candidate multiferroic material
Charge, spin and orbital order in the candidate multiferroic material

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Physics of Magnetically Confined Plasmas

... plasma processes rather than by electromagnetic radiation. Confined plasmas are usually, but not always, in a state in which microturbulence dominates the transport processes. Microturbulence, Section (VI.F), means the fluctuations have a wavenumber that is of order of the inverse of an ion gyroradi ...
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coordination scope, sequence - Scope, Sequence, and Coordination

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Decoherence and the Transition from Quantum to Classical–Revisited
Decoherence and the Transition from Quantum to Classical–Revisited

... subsystems. There can be no observer “on the outside.” In this universal setting, classicality must be an emergent property of the selected observables or systems. At first glance, the Many Worlds and Copenhagen Interpretations have little in common. The Copenhagen Interpretation demands an a priori ...
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B.Sc.PHYSICS(HONOURS) PART I(SEMESTER

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MAGNETIC FIELDS IN NEUTRON STARS Daniele Viganò

... This work aims at studying how magnetic fields affect the observational properties and the long-term evolution of isolated neutron stars, which are the strongest magnets in the universe. The extreme physical conditions met inside these astronomical sources complicate their theoretical study, but, th ...
The effect of material properties to electric field
The effect of material properties to electric field

Path Integrals — Elementary Properties and Simple Solutions
Path Integrals — Elementary Properties and Simple Solutions

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Coupled Quantum Dots — Spatial Correlations between Interacting

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I. Results from Prior NSF Support

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80, 032307 (2009)

Chapter 21 The Electric Field I: Discrete Charge Distributions
Chapter 21 The Electric Field I: Discrete Charge Distributions

... A popular classroom demonstration consists of rubbing a plastic rod with fur to give the rod charge, and then placing the rod near an empty soda can that is on its side (Figure 21-36). Explain why the can will roll toward the rod. Determine the Concept Because the can is grounded, the presence of th ...
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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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