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Magnetic-field-induced Anderson localization in a strongly
Magnetic-field-induced Anderson localization in a strongly

HW 4 solutions
HW 4 solutions

Lecture 33
Lecture 33

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... Weak measurements: from the 3-box problem to Hardy's Paradox to the which-path debate • The 3-box problem • Another case where airtight classical reasoning yields seemingly contradictory information • Experimental consequences of this information • Actual experiment! • Weak measurements shed light o ...
hw03_solutions
hw03_solutions

... 9. How does the energy stored in a capacitor change if (a) the potential difference is doubled, and (b) the charge on each plate is doubled, as the capacitor remains connected to a battery? Solution (a) The energy stored in the capacitor is given by equation, PE  12 CV 2 . Assuming the capacitance ...
r. - q P,
r. - q P,

... 27. An electron moving with a speed of 4.86 x 106 m/s is shot parallel to a uniform electric field of strength 1030 N/C arranged so as to retard its motion. (a) How far will the electron travel in the field before coming (momentarily) to rest and (b) how much time will elapse? (c) If the electric fi ...
hw03_solutions
hw03_solutions

Electric Charge And Static Electricity
Electric Charge And Static Electricity

Class XII worksheet- 4 Magnetic effects of current and Magnetism /V
Class XII worksheet- 4 Magnetic effects of current and Magnetism /V

Electrostatics Practice Test Which one of the following represents
Electrostatics Practice Test Which one of the following represents

Chapter 20 Concept Tests - University of Colorado Boulder
Chapter 20 Concept Tests - University of Colorado Boulder

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PHYS 241 Exam Review

Physics 386 Practice Hour Exam 1
Physics 386 Practice Hour Exam 1

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Ch 4: Potential Difference and Ch 4

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Electric fields in matter

648 CHAPTER 17. ELECTRIC POTENTIAL ENERGY AND THE
648 CHAPTER 17. ELECTRIC POTENTIAL ENERGY AND THE

Physics 2135 Exam 1
Physics 2135 Exam 1

... Five multiple choice questions, 8 points each. Choose the best or most nearly correct answer. _____1. A proton and an electron are at rest in a constant electric field created by oppositely charged conducting plates. You release the proton from the positive plate and the electron from the negative p ...
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Class Notes - December 4

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Lecture 8 Magnetic Fields

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REC 4 - Department of Physics and Astronomy : University of

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WHAT IS A PHOTON? Spontaneous emission

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Chapter 20 Magnetic Forces and Magnetic Fields

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Solutions to Assignment 5 1. a) From the relations F=mv2/r and F

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LS50 pset 9

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Midterm 4 Statistics

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< 1 ... 543 544 545 546 547 548 549 550 551 ... 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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