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Manual.
Manual.

How can a 22-pole ion trap exhibit ten local minima
How can a 22-pole ion trap exhibit ten local minima

Word
Word

Applied Nonlinear Optics
Applied Nonlinear Optics

iBios – Portal Project Integrative Toolbox Using Grid
iBios – Portal Project Integrative Toolbox Using Grid

Application of the underscreened Kondo lattice model to neptunium
Application of the underscreened Kondo lattice model to neptunium

... Thus, with decreasing temperature, there is first a ferromagnetic state between TC and TK and then a mixed Kondo-ferromagnetic state below TK with a clear decrease of the ferromagnetic magnetization. In the ferromagnetic phase, the magnetic moment is almost saturated, reaching a value close to 1. In ...
EXAM 1
EXAM 1

... Show all work!! Report all numbers to three (3) significant figures. A point charge q = 20.0 nC is located at the center of a unifonn ring having linear charge density A. = -10.0 nC/m and radius a = 0.50 m, as shown in the figure. Detennine the total outward electric flux through a sphere centered a ...
The Microwave Hall Effect Measured Using a Waveguide Tee J. E.
The Microwave Hall Effect Measured Using a Waveguide Tee J. E.

... coherent microwaves at high powers. Coaxial cables are now much more widely used than metal waveguides, but in this experiment we use X band waveguides because we are able to cut a slot to insert a sample into a waveguide series tee. There are two main methods for measuring the microwave Hall effect ...
CHAPTER 5 5.1. Given the current density J = −104[sin(2x)e−2y ax
CHAPTER 5 5.1. Given the current density J = −104[sin(2x)e−2y ax

Is the electron a photon with toroidal topology?
Is the electron a photon with toroidal topology?

Electromagnetic Levitation Thesis
Electromagnetic Levitation Thesis

Model for the magnetoresistance and Hall coefficient of inhomogeneous graphene 兲
Model for the magnetoresistance and Hall coefficient of inhomogeneous graphene 兲

... greater than about 1 T. At f n = 0.5, ␳xy = 0 for all B. Within the present model, this latter result is exact, and not restricted to the EMA.10 Figure 3 shows ␳xx共B , f n兲 versus f n for several values of B. We use the EMA and the same parameters as in Figs. 1 and 2 共with ␻c␶ = 2.3B兲. ␳xx saturates ...
Fine Structure of the Hydrogen Atom. Part I
Fine Structure of the Hydrogen Atom. Part I

Silicon quantum electronics
Silicon quantum electronics

... at the same time. Furthermore, states of different qubits can be entangled with each other. This means that the outcome of a measurement on one of the entangled qubits will influence the outcome of a measurement on the other, irrespective of how far the qubits are apart. There are detailed theoretic ...
Majorana Fermions - Physics | Oregon State University
Majorana Fermions - Physics | Oregon State University

... Majorana fermions. Ideal probes of these excitations are inelastic neutron scattering experiments. These we report here for a ruthenium-based material, α-RuCl3, continuing a major search (so far concentrated on iridium materials) for realizations of the celebrated Kitaev honeycomb topological QSL. O ...
Problems in nucleon structure study
Problems in nucleon structure study

Electrical Energy and Capacitance
Electrical Energy and Capacitance

Cross-field flow and electric potential in a plasma slab
Cross-field flow and electric potential in a plasma slab

MFF 3a: Charged Particle and a Straight Current
MFF 3a: Charged Particle and a Straight Current

Review 2: Many True/False
Review 2: Many True/False

Ten Years of Spin Hall Effect
Ten Years of Spin Hall Effect

Magnetostriction of GdAg2, PrFe4As12, and GdVO3 measured with
Magnetostriction of GdAg2, PrFe4As12, and GdVO3 measured with

Antiferroelectric Shape Memory Ceramics
Antiferroelectric Shape Memory Ceramics

... Ceramics “shape memory” has also been reported for certain ferroelectricity-related transitions, namely paraelectric–ferroelectric [11] and antiferroelectric (AFE)–ferroelectric (FE) transitions [12,13]. The former thermally-induced transition revealed a shape-recovery phenomenon similar to zirconia ...
1 Transport of Dirac Surface States
1 Transport of Dirac Surface States

Josephson junctions
Josephson junctions

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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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