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Superconducting qubits coupled to nanoelectromechanical resonators: An architecture
Superconducting qubits coupled to nanoelectromechanical resonators: An architecture

Applied Bohmian mechanics
Applied Bohmian mechanics

... After these two sets of examples on Bohmian applications, in Section 4, we discuss the original routes, i.e. the formalism, opened by the Bohmian theory. For example, the trajectories can be computed from the Schrödinger or from the Hamilton-Jacobi equations. See the mathematical differences in Sect ...
Quantum Computation and Quantum Information 10th Anniversary
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Quantum Fields on BTZ Black Holes

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Theories of Experimentally Observed Excitation

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Physics II Exam 2 Review

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Magnetization reversal in magnetic films

... magnetic properties of Co and Co alloy thin films has been studied in detail. Hereby, an epitaxially grown 30 nm thick (1010) Co thin film, which has in-plane uniaxial magnetic anisotropy, has been utilized as a reference structure due to its simple and well-understood behaviour. In order to modify ...
Applying elementary principles from quantum physics
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Design of Powder Core Motors - IEA

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electromagnetic damping

... We must consider the equation for two intervals: 0 < t < τ and τ < t < ∞. During the first of these intervals, the coil acquires momentum due to impulse given to it by transient current. It, however, is hardly deflected from its initial position because of the stipulation that the transient current ...
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Wound pH depends on actual wound size

Ultracold collisions in traps - EDOC HU - Humboldt
Ultracold collisions in traps - EDOC HU - Humboldt

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Coherent Control of Polarized Neutron Interferometry

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A Lightning Parameterization for Numerical Cloud Models - storm-t

... have been modified: 1) To account for subgrid-scale variations, the initiation point is chosen randomly from among grid points at which the electric field magnitude is above a threshold value, instead of being assigned always to the grid point having the maximum electric field magnitude. 2) The thre ...
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Matched Distributions in Cyclotrons with Higher Order Moments of

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Quantum Theory of Condensed Matter (260 Pages)

... Conference on Physics. It is true, as David suggested, that I was rather hesitant at first to take on this responsibility. The prospect of trying to choose fifty participants to represent a field as broad as condensed matter physics seemed especially daunting. In organizing the conference, I did ind ...
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Inhaltsverzeichnis • Contents - the Max Planck Institute for the

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1. Introduction 1.1 Scope of the Course 1.2 Introduction to the Course

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Archived Qualifying Exam Problems - UW SharePoint
Archived Qualifying Exam Problems - UW SharePoint

Central region study for a moderate energy cyclotron
Central region study for a moderate energy cyclotron

Bose-Einstein Condensation of Molecules
Bose-Einstein Condensation of Molecules

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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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