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Implementations of Quantum Information
Implementations of Quantum Information

Broken symmetry revisited - Homepages of UvA/FNWI staff
Broken symmetry revisited - Homepages of UvA/FNWI staff

Midterm Exam No. 01 (Spring 2015)
Midterm Exam No. 01 (Spring 2015)

... Using Eq. (10), determine G0 (r, 0) in terms of a single integral. That is, evaluate the sum for this case. 5. (20 points. Take home exercise, to be submitted during exam.) Consider a spherical cavity of radius a with perfectly conducting walls that is grounded. The inside of the cavity is described ...
Dissecting the Higgs Discovery: The Anatomy of a 21st Century
Dissecting the Higgs Discovery: The Anatomy of a 21st Century

Hall effect for p type semiconductor
Hall effect for p type semiconductor

JOURNAL OF MODERN OPTICS, 1987, VOL . 34, NO. 11, 1401
JOURNAL OF MODERN OPTICS, 1987, VOL . 34, NO. 11, 1401

twopointcharges01
twopointcharges01

... Two more +Q charges are held in place the same distance s away from the +q charge as shown. Consider the following student dialogue concerning the net force on the +q charge: Student 1: “The net electric force on the +q charge is now three times as large as before, since there are now three positive ...
twopointcharges01 by AJC2012
twopointcharges01 by AJC2012

Electric Field
Electric Field

Notes for Unit
Notes for Unit

Chapter 17 clicker questions
Chapter 17 clicker questions

... Which of the following statements is NOT correct about the magnetic dipole moment? a) The direction of the dipole moment vector is perpendicular to the surface of the loop. b) The bigger the dipole moment, the greater the torque that an external magnetic field exerts on it. c) The magnetic dipole mo ...
Physics 416G : Solutions for Problem set 7
Physics 416G : Solutions for Problem set 7

... a) Sketch n+ (z) and n(z) on the same graph and give a physical explanation of why they might be reasonable description of a metal surface. b) Calculate the dipole moment p~ per unit area of surface for this system. c) Calculate the electrostatic potential φ(z) and sketch it in the interval −∞ < z < ...
Practical Electromagnetic Shielding
Practical Electromagnetic Shielding

... In order to power and/or communicate with the electronics in a shielded enclosure, it is often necessary to emplo through the enclosure wall. A single unshielded, unfiltered wire penetrating a shielded enclosure can completely shielding benefit that the enclosure otherwise provided. As illustrated i ...
Precision spectroscopy with two correlated atoms
Precision spectroscopy with two correlated atoms

Phys132Q Lecture Notes - University of Connecticut
Phys132Q Lecture Notes - University of Connecticut

Motors and Generators
Motors and Generators

... perform an investigation to model the behaviour of semiconductors, including the creation of a hole or positive charge on the atom that has lost the electron and the movement of electrons and holes in opposite directions when an electric field is applied across the semiconductor ...
Interacting electrons in a magnetic field: Mapping quantum
Interacting electrons in a magnetic field: Mapping quantum

Group Problems #36 - Solutions Monday, November 28 Problem 1 Transition Selection Rules
Group Problems #36 - Solutions Monday, November 28 Problem 1 Transition Selection Rules

... x. For the current perturbation, W = eξx, this means that ψn and ψm must have opposite parity (i.e., if one is even the other must be odd) so that the integrand is even. Note that the product of two even functions is even, the product of two odd functions is even, and the product of an even and an o ...
Physics - Electrostatics Tutorial Question 1 – Fun with Tape a) Press
Physics - Electrostatics Tutorial Question 1 – Fun with Tape a) Press

... Pip and Jed are playing a game of Pig-In Pig-Out. The players draw charged stones from a bag and place them on the board. The first player (Jed) tries to place stones so that the pig will be in an electric field, while the second player (Pip) tries to place stones so that there is no net field where ...
Sample Quiz 1 - U of M Physics
Sample Quiz 1 - U of M Physics

... (D) not enough information MC2 Two identical conducting spheres A and B carry equal charge. They are separated by a distance much larger than their diameters. A third identical conducting sphere C is uncharged. Sphere C is first touched to A, then to B, and finally removed. As a result, the electros ...
HW1 solutions
HW1 solutions

Continuity Equation
Continuity Equation

... Excess carriers in s/c cause non-equilibrium condition, where most of s/c devices operate under this circumstances. Carriers may be generated by: forward-bias of p-n junction, incident light, and impact ionization. Continuity equation – the governing equation for the rate of charge carriers. Thermio ...
Uncertainty Principle
Uncertainty Principle

phys1444-lec5
phys1444-lec5

... Solution: a. The electric fields add in magnitude, as both are directed towards the negative charge. E = 6.3 x 108 N/C. b. We don’t know the relative lengths of E1 and E2 until we do the calculation. The acceleration is the force (charge times field) divided by the mass, and will be opposite to the ...
paper -2003
paper -2003

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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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