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Chapter 16
Chapter 16

Quantizing charged magnetic domain walls: Strings on a lattice
Quantizing charged magnetic domain walls: Strings on a lattice

chapter 5
chapter 5

... which Ψ(x,t)2 will give us the probability of finding the particle of the matter wave there (x) and then (t) Ψ(x,t) contains everything that is and can be know about the particle, to get the probability of finding the particle at some specific (x,t) we have to calculate Ψ(x,t)2 Born’s interpretation ...
(Electrostatics in Biology)
(Electrostatics in Biology)

On the consequences of bi-Maxwellian distributions on parallel electric fields.
On the consequences of bi-Maxwellian distributions on parallel electric fields.

... maximum at the equator and the equatorially trapped plasma is confined closer to the equator for higher anisotropy ratios. The modeled density profiles are in agreement with some observations. The electric fields that result are on the order of 0.1 uV/m pointing away from the magnetic equator with g ...
There had been developed a firm construct of the
There had been developed a firm construct of the

COLD ATOMS AND CREATION OF NEW STATES OF MATTER: BOSE-
COLD ATOMS AND CREATION OF NEW STATES OF MATTER: BOSE-

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Mechanical rotation of nanomagnet through interaction with an

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The Historical and Conceptual Development of
The Historical and Conceptual Development of

BEC and optical lattices
BEC and optical lattices

functions and (so-called px- and py-orbitals) are linear combinations
functions and (so-called px- and py-orbitals) are linear combinations

NB Electric Field Hockey
NB Electric Field Hockey

Electrostatics
Electrostatics

... the positively charged ions on the unexposed areas on the drum's surface attractive. The same particles are subsequently even more drawn to the electrostatically charged  paper. The plastic in the toner lets you keep it from jumping ship once you've finally got  it on the paper; all you have to do i ...
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pen14qip

Tesla Healing Technology - Breakthru
Tesla Healing Technology - Breakthru

PH202 chapter 20 solutions
PH202 chapter 20 solutions

Transverse transport in disordered superconducting films above T_c
Transverse transport in disordered superconducting films above T_c

... D (Hubbard-Stratonovich transformation): ...
Electric Forces and Fields
Electric Forces and Fields

Document
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p-shell hybridization and Hund`s-rule mitigation
p-shell hybridization and Hund`s-rule mitigation

Quantum Mechanics and Chaos Theory
Quantum Mechanics and Chaos Theory

... on the table and the consequent trajectory that the particle follows around the table. If the initial point is displaced and the shot now taken from this new initial point at the same angle as before, we see that the particle follows a new trajectory that remains a constant distance from the previou ...
EE 4BD4 2013 Lecture 3
EE 4BD4 2013 Lecture 3

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META10 Sendur

... between two surfaces at small gaps. Rousseau et al. [11] investigated an experimental setup that can measure the conductance when the objects are separated by varying the distances between 30 nm and 2.5 µm. The experimental data by Rousseau et al. [11] confirms the theoretical results that the near- ...
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... A function f : [a, b] → R is said to be generalized Riemann integrable on [a, b] if there exists a number L ∈ R such that for every  > 0 there exists a gauge δ on [a, b] such that if Ṗ is any δ -fine partition of [a, b], then |S(f ; Ṗ) − L| < , where S(f ; Ṗ) is any Riemann sum for f using t ...
< 1 ... 230 231 232 233 234 235 236 237 238 ... 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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