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Part 5. Semiconductors
Part 5. Semiconductors

chapter22 - galileo.harvard.edu
chapter22 - galileo.harvard.edu

The Electric Field
The Electric Field

topological phase transitions and topological
topological phase transitions and topological

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a16.3Physics Section 16.3

... 1. Electric field lines originate from a positively charged object and terminate at a negatively charge object. 2. Electric field lines originate and terminate perpendicular to the surface of a charged object. 3. The density of the electric field lines indicate the strength of the electric field. 4. ...
Electric Potential
Electric Potential

Quantum Control in Cold Atom Systems
Quantum Control in Cold Atom Systems

Chap. 16 Conceptual Modules Giancoli
Chap. 16 Conceptual Modules Giancoli

****** 1 - Weizmann Institute of Science
****** 1 - Weizmann Institute of Science

Applications of Coherence by Identity
Applications of Coherence by Identity

... Quantum Interference “A phenomenon which is impossible, absolutely impossible, to explain in any classical way, and which has in it the heart of quantum mechanics.” – Feynman ...
AP Physics Electricity
AP Physics Electricity

... up on the outer surface of the metal enclosure. Due to a combination of q and r at any point within the box, cylinder, sphere, etc. the electric field is zero inside. E = 0. This is why you are not electrocuted in a car or airplane if it is struck by lightening. ...
Chapter 2 Plane Waves and Refractive Index
Chapter 2 Plane Waves and Refractive Index

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2 Properties of 3jm- and 3nj-Symbols

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Quantum-electrodynamical approach to the Casimir force
Quantum-electrodynamical approach to the Casimir force

... given rise to numerous subsequent studies [3], most of them based on intricate mathematical extrapolation methods. Another way, chosen by some authors for computing the Casimir force, consists in writing down an expression derived directly from Maxwell’s stress tensor instead of differentiating the ...
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could

Understanding Electron Spin
Understanding Electron Spin

Physical Chemistry (4): Theoretical Chemistry
Physical Chemistry (4): Theoretical Chemistry

... At the turning of the 19th and 20st century new experiments appeared which could not be explained by the tools of the classical (Newtonian) mechanics. For the new theory new concepts were needed: • quantization: the energy can not have arbitrary value • particle-wave dualism ⇒ development of QUANTUM ...
Electric potential energy and electric potential
Electric potential energy and electric potential

Related Solved Problems and Other Problems
Related Solved Problems and Other Problems

Quantum Transport and its Classical Limit
Quantum Transport and its Classical Limit

... If m=n: also contribution if b = a timereversed of a: Without magnetic field: a and a have equal actions, hence Factor-two enhancement of diagonal reflection ...
MT144_001 - WordPress.com
MT144_001 - WordPress.com

Optical lattices - Condensed Matter Theory and Quantum Optics
Optical lattices - Condensed Matter Theory and Quantum Optics

Basic Electrostatics
Basic Electrostatics

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L6 Lorentz force

< 1 ... 393 394 395 396 397 398 399 400 401 ... 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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