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Experimental Generation and Manipulation of Quantum Squeezed
Experimental Generation and Manipulation of Quantum Squeezed

Design, Development and Operation of Novel Ion Trap Geometries
Design, Development and Operation of Novel Ion Trap Geometries

... 1.18 Schematic diagram of a non-resonant electronic detection scheme coupled into an ion trap. . . . . . . . . . . . . . . . . . . . . . 47 1.19 Schematic diagram of a resonant electronic detection scheme coupled into an ion trap. . . . . . . . . . . . . . . . . . . . . . 48 1.20 Resonant response o ...
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Non-collinear Magnetoelectronics Abstract

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PhD thesis - Paul G. Evans Research Group

... For this work, synchrotron x-ray microdiffraction was used to study polarization switching, polarization fatigue, and piezoelectricity in epitaxial PZT thin film capacitors. Polarization domains can be visualized based on the change in the intensity of the PZT {002} Bragg reflections due to polariza ...
Relativistic Quantum Information: developments in Quantum
Relativistic Quantum Information: developments in Quantum

... description of gravity: mass and energy move in a curved spacetime and the spacetime is curved by the presence of mass and energy. However, it is far from being complete. General relativity allows ill-defined objects such as singularities, and in the presence of a singularity it loses its predictive ...
Plasma and trap-based techniques for science with positrons
Plasma and trap-based techniques for science with positrons

... on both that work and work with electrons to create a variety of intense radiation sources, such as traveling wave tubes and klystrons (Pierce, 1954). From those and many other plasma studies, it became clear that relatively dense and cool collections of trapped charge particles exhibit a range of p ...
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pdf - arXiv

2001 by CRC Press LLC
2001 by CRC Press LLC

ABSTRACT PHENOMENOLOGICAL ASPECTS OF HEAVY QUARK SYSTEMS
ABSTRACT PHENOMENOLOGICAL ASPECTS OF HEAVY QUARK SYSTEMS

... couplings. The large couplings prevent a meaningful perturbative expansion in powers of the strong coupling constant for low energy hadronic physics. This lack of a perturbative expansion greatly complicates hadronic calculation from the fundamental principles of QCD and necessitates the use of non- ...
O A RIGINAL RTICLES
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... and when the motion in all three dimensions is confined, and we talk about a quantum dot. In solid state engineering, these are commonly called low dimensional quantum structures. Carbon demonstrates unusually complicated behavior, forming a number of very different structures. However, only three-d ...
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Define resistance V splitting between components V

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Topological phases and polaron physics in ultra cold quantum gases
Topological phases and polaron physics in ultra cold quantum gases

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Table of Contents - Precision Muon Physics

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Electrical Manipulation and Detection of Single Electron Spins in

... the happy dance alive! Thanks for all the enthusiasm, happiness and great teamwork. And, if you dont mind, I would still really like to learn this specific dance... Tristan, discussions with you were always interesting and exciting, regardless if it was on physics or any other topic (5 minutes???). I ...
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Physical Processes in Protoplanetary Disks

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Quantum computation and quantum information (PDF

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Lecture Notes 18.5: Lorentz Transformation of EM Fields, the EM

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Quantum Hall Effect and Electromechanics in Graphene

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Escape from a metastable state - Physik Uni

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Design, synthesis and study of coordination complexes for quantum computing

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Electronic and transport properties of nanotubes

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Magnetic vortex dynamics induced by an electrical current

Physics 505 Fall 2007 Homework Assignment #4 — Solutions
Physics 505 Fall 2007 Homework Assignment #4 — Solutions

< 1 2 3 4 5 6 7 ... 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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