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E1344: Oscillations between a site and a ring
E1344: Oscillations between a site and a ring

... A given ring with length L = 1 has N sites, which have equal potential (V = 0). The hopping amplitude of a particle per time unit between neighbouring sites is c. Another site is added at the center of the ring. The relation energy of the particle in the central site is ε0 . The hopping amplitude pe ...
127 Magnetic monopole and magnetic charge
127 Magnetic monopole and magnetic charge

... we had to formulate: „There are no particles for which the volume integral of the divergence of the magnetic field strength over a region of space that contains the particle is different from zero.“ By the way, one could get rid of the electric charge in the same way. Obviously nobody would do so. O ...
Comment on `About the magnetic field of a finite wire`
Comment on `About the magnetic field of a finite wire`

Advanced Level Physics - Edexcel
Advanced Level Physics - Edexcel

... total mark for this paper is 80. t The marks for each question are shown in brackets t The – use this as a guide as to how much time to spend on each question. Questions labelled with an asterisk (*) are ones where the quality of your ...
Jackson 4.10 Homework Problem Solution
Jackson 4.10 Homework Problem Solution

Quantum ElectroDynamics
Quantum ElectroDynamics

Electric Shielding and the Electric Field
Electric Shielding and the Electric Field

Electric Shielding and the Electric Field
Electric Shielding and the Electric Field

... Electric Shielding and the Electric Field Speaking of induction, we discussed a simple experiment with the ball on the silk thread and the charged rod. We saw that they affected each other at a distance. A similar effect is produced by magnets. We call the region of influence of magnetic forces surr ...
Exercise 1
Exercise 1

Activity 4 – Induction in an Aluminum Can
Activity 4 – Induction in an Aluminum Can

... In this activity, Lenz’s Law is demonstrated. Lenz’s Law states that an induced electromotive force generates a current that induces a counter magnetic field that opposes the magnetic field generating the current. In this activity, an empty aluminum can floats on water in a tray, such as a Petri dis ...
Background 2
Background 2

Physics - Kendriya Vidyalaya, Gill Nagar
Physics - Kendriya Vidyalaya, Gill Nagar

... Name the part of electromagnetic spectrum to which these radiations belong. Arrange these wavelengths in decreasing order of their magnitude. 23. A convex lens, of focal length 20cm, is placed coaxially with a convex mirror of radius of curvature 20cm. The two are kept 15cm apart from each other. A ...
Adding magnetic fields
Adding magnetic fields

Goal: To understand what Electric Fields are
Goal: To understand what Electric Fields are

... • So, the more loops, the more voltage you have on that side. • That is why the ratio of voltages was the ratio of the # of loops! ...
8.3 Electrical Energy in the Home
8.3 Electrical Energy in the Home

hw06_solutions
hw06_solutions

... The force on the segment of the loop closest to the wire is towards the wire, since the currents are in the same direction. The force on the segment of the loop farthest from the wire is away from the wire, since the currents are in the opposite direction. Because the magnetic field varies with dist ...
You may use your equation sheet on this exam
You may use your equation sheet on this exam

The History of Quantum Mechanics
The History of Quantum Mechanics

L143.2 - Duke Physics
L143.2 - Duke Physics

Quantum Rings with Two Deeply Bound Electrons under a Magnetic
Quantum Rings with Two Deeply Bound Electrons under a Magnetic

... Quantum rings are a kind of well-known mesoscopic systems having a great potential application.[1−6] Since their physical properties can be controlled, the physics involved is very rich, therefore they are also attractive in the academic aspect. Now the quantum rings containing only a few electrons ...
Practice Problems without Answers Part 2 rev 4
Practice Problems without Answers Part 2 rev 4

Physics 202-Section 2G Worksheet 1- Electrostatic force and electric
Physics 202-Section 2G Worksheet 1- Electrostatic force and electric

Lecture 19
Lecture 19



... farther away from a certain field point contribute less. The units of A are kgm/(Csec). Note that it is not a potential energy. It is sometimes referred to as a potential momentum. The field A shows up in the Hamiltonian when doing quantum mechanics. We will explain the meaning of A in a future chap ...
August 28 /29th th Electric Fields
August 28 /29th th Electric Fields

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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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