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Massachusetts Tests for Educator Licensure (MTEL )
Massachusetts Tests for Educator Licensure (MTEL )

Quantum computing with photons: introduction to the circuit model
Quantum computing with photons: introduction to the circuit model

Bulk and Structure Inversion Asymmetry in Semiconductor Quantum
Bulk and Structure Inversion Asymmetry in Semiconductor Quantum

1901 – 1921
1901 – 1921

An assessment of the role of the centrifugal acceleration mechanism
An assessment of the role of the centrifugal acceleration mechanism

... The centrifugal acceleration is however of a more general importance. Its role has been discussed also for other planets. Delcourt et al. (2002) investigated the centrifugal acceleration near Mercury. Haider (1996) discussed the role of the polar wind and associated centrifugal acceleration of ions ...
Physical Foundations of Quantum Electronics
Physical Foundations of Quantum Electronics

Non-Abelian Anyons and Topological Quantum Computation
Non-Abelian Anyons and Topological Quantum Computation

... particles are interchanged twice in a clockwise manner, their trajectory involves a non-trivial winding, and the system does not necessarily come back to the same state. This topological difference between two and three dimensions, first realized by Leinaas and Myrheim, 1977 and by Wilczek, 1982a, l ...
MOLECULAR DYNAMICS SIMULATION OF A NANOSCALE
MOLECULAR DYNAMICS SIMULATION OF A NANOSCALE

... 1. Nanoscale sequencing device concept developed by researchers at ORNL................... 6 2. Proposed synchronization and coordination of applied electric fields........................... 9 3. A top view shown without the upper mica plate for clarity and side view of the sequencing device initia ...
Contributions to the Quantum Optics of Multi
Contributions to the Quantum Optics of Multi

the problem book
the problem book

... c. Writing Ψ(x) = φ(x)f (x), find the differential equation that determines f (x). ...
PARKER WORKSHOP ON MAGNETIC RECONNNECTION
PARKER WORKSHOP ON MAGNETIC RECONNNECTION

spin - Groups - Texas A&M University
spin - Groups - Texas A&M University

Bulk Entanglement Spectrum Reveals Quantum
Bulk Entanglement Spectrum Reveals Quantum

... subsystem A. Using the exponential decay of Cðr; r0 Þ at large distance jr − r0 j, we prove [28] that HA is short ranged and resembles a physical Hamiltonian, provided that the volume of A does not exceed that of B. In the opposite case, HA has bands at ∞ [28]; nonetheless, the low-lying part of th ...
Atomic Physics Division Fachverband - DPG
Atomic Physics Division Fachverband - DPG

... partners to be either in the separable, entangled, or Bell correlated regions. The symmetry of the scattering process allows for the construction of explicit examples applying methods of classical communication and local operations for illustrating the concepts of nonlocality versus separability. It ...
Macroscopic Models of Superconductivity
Macroscopic Models of Superconductivity

accelerators for physics experiments: from diagnostics
accelerators for physics experiments: from diagnostics

PDF - 8MB - MIT OpenCourseWare
PDF - 8MB - MIT OpenCourseWare

... These experiments showed that when a charged conductor contacted another conductor , whether charged or not. the total charge on both bodies was shared. The presence of charge was first qualitatively measured by an electroscope that consisted of twO attached metal foil leaves. When charged. the mutu ...
Semiclassical model of stimulated Raman scattering in photonic crystals * Lucia Florescu
Semiclassical model of stimulated Raman scattering in photonic crystals * Lucia Florescu

... scattering 关13,14兴, or considered the stimulated Raman scattering 共SRS兲 in one-dimensional photonic crystals 关15兴. Specifically, a quantum theory of resonance Raman scattering of light from an atomic system embedded in a photonic bandgap material has been developed 关13兴. This theory enables the inve ...
Quantum Structures
Quantum Structures

Wave Propagation through Vegetation at 3.1 GHz and 5.8 GHz
Wave Propagation through Vegetation at 3.1 GHz and 5.8 GHz

Circuit QED: Superconducting Qubits Coupled to
Circuit QED: Superconducting Qubits Coupled to

The Heisenberg antiferromagnet on the square
The Heisenberg antiferromagnet on the square

Quantifying particle motion under force fields in
Quantifying particle motion under force fields in

Electrospinning and electrically forced jets. I. Stability theory
Electrospinning and electrically forced jets. I. Stability theory

... the onset of electrospinning always corresponds with the whipping of the jet. The goal of this series of papers is to develop a theoretical framework for understanding the physical mechanisms of electrospinning, and to provide a way of quantitatively predicting the parameter regimes where it occurs. ...
Chapter 22 The Electric Field II: Continuous Charge
Chapter 22 The Electric Field II: Continuous Charge

... (a) From the application of Gauss’s law we know that the electric field in this region is not zero. A positively charged object placed in the region for which r < R1 will experience an attractive force from the charge –Q located at the center of the shell. Hence the direction of the electric field i ...
< 1 ... 13 14 15 16 17 18 19 20 21 ... 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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