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Localization, interaction and the modern interpretation(s) of quantum mechanics
Localization, interaction and the modern interpretation(s) of quantum mechanics

... multifractality arise without internal contradictions as the Bohm trajectories are not allowed to cross each other. The comparison of the trajectories to the semi-classical characteristics such as scar states, etc., should also be most interesting, particularly their variation with magnetic flux. In ...
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equipotential surface

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... evidenced by the areas of green glow around the shape of the cross. This showed that the rays travelled in straight lines. The paddle wheel must be pushed by a particle with momentum if it is to start rolling. 19. An electron entering an electric field will experience a force in ...
“Step-induced defects in thin films and the properties”
“Step-induced defects in thin films and the properties”

CHEMISTRY CHAPTER 4 – QUANTUM MECHANICS
CHEMISTRY CHAPTER 4 – QUANTUM MECHANICS

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Examples of Magnetic Fields

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... 21. How can the electrical potential energy of a charged particle in an electric field be increased? ...
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... ! Arrow gives direction ! Leave +, North ! Enter -, South Differences ! Start/Stop on electric charge ! No Magnetic Charge ! lines are continuous! ...
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... If you took an electrically charged ball and shook it up and down rapidly, charges in a nearby metal object would move in response. How far away could that metal object be and still respond? 1. 1 meter 2. 1 kilometer 3. The other side of the universe ...
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Eddy currents - University of Iowa Physics

Electric Fields
Electric Fields

... Magnitude of E determined form the electric potential difference  Weight of electron had to be determined  Drop was suspended and then the electric field was turned off so the drop could fall  Because friction of tiny drop so large terminal velocity was reached quickly  Using a complex equation ...
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Unit 10 Worksheet 5

... 2. Calculate the gravitational potential difference between: a) point A and the base of the hill b) point B and the base of the hill c) point C and point A d) point C and point E e) Would an object gain more energy going from D to A or from E to F? Why? ...
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Magnetic Field Lines, sketch Magnetic Field Lines, Bar Magnet

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Chapter 22 Lecture Notes 1.1 Changing Electric Fields Produce

Physics 2102 Lecture 15
Physics 2102 Lecture 15

< 1 ... 615 616 617 618 619 620 621 622 623 ... 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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