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20041014090010101-148859
20041014090010101-148859

Ground states of helium to neon and their ions in strong magnetic
Ground states of helium to neon and their ions in strong magnetic

Energy and angular distributions of electrons resulting from barrier
Energy and angular distributions of electrons resulting from barrier

Fundamentals of NMR
Fundamentals of NMR

PDF
PDF

... order can be broken locally on a point or along a line, generating a singularity for the director field. In analogy with the dislocations in a crystal, nematic line defects are named disclinations. The disclinations are topological objects and are often classified according to their strength which c ...
Collisional properties of ultracold potassium
Collisional properties of ultracold potassium

... owing to its small scattering length. This problem will be exacerbated if the scattering lengths turn out to be negative. Figure 1 illustrates this point, by showing the energydependent s-wave cross sections for u 22& 1 u 22& collisions. For a small positive value of a t (39), the cross section rema ...
10 10-0
10 10-0

... With the magnetic field pointing downward and the area vector A pointing upward, the magnetic flux is negative, i.e., ! B = " BA < 0 , where A is the area of the loop. As the magnet moves closer to the loop, the magnetic field at a point on the loop increases ( dB / dt > 0 ), producing more flux thr ...
First results of the new type of measurements of atmospheric electric
First results of the new type of measurements of atmospheric electric

Chapter 1 Fundamentals of NMR
Chapter 1 Fundamentals of NMR

... SUMMARY The general phenomenon of nuclear magnetic resonance is introduced using both a classical and a quantum mechanical perspective. This provides the basis for understanding measurable and informative NMR parameters: chemical shift, spin-spin splitting, linewidths, relaxation, the nuclear Overha ...
OpenStax_Physics_CH18_ImageSlideshow
OpenStax_Physics_CH18_ImageSlideshow

Are dark fringes devoid of energy of the
Are dark fringes devoid of energy of the

Quantum Spin Hall Effect and Enhanced Magnetic Response by
Quantum Spin Hall Effect and Enhanced Magnetic Response by

The Millikan Experiment
The Millikan Experiment

Arc Attack - Society for the Performing Arts
Arc Attack - Society for the Performing Arts

... around it that your nose can detect. A field is a three-dimensional description of a region of space. In this case, the field your nose detects is that created by the odorous molecules from the trash. If there are more odorous molecules, the field is stronger, and you can tell! If there aren’t very ...
Jackson 1.1 Homework Problem Solution
Jackson 1.1 Homework Problem Solution

... And since the surface A can be drawn anywhere in the hollow region, the electric field must be zero everywhere in the hollow region. The shell therefore shields the hollow region from external fields and charges. We have shown: Concept 5. The electric field everywhere inside the hollow region of a c ...
The Millikan Experiment
The Millikan Experiment

magnetic circuit design
magnetic circuit design

... curve, the magnetic field distribution on the outside of the magnet, assuming the space of length X and the same cross section shape with permeability equal to the magnet, is similar to the magnetic field generated by the closed circuit current on the outer surface. ...
Voltage and Capacitance Electric Potential Energy Electric Work
Voltage and Capacitance Electric Potential Energy Electric Work

Module P4.2 Introducing magnetism
Module P4.2 Introducing magnetism

Complete electromagnetic multipole expansion including toroidal
Complete electromagnetic multipole expansion including toroidal

... The electromagnetic multipole expansion presented in this paper is complete on two accounts: i) It is valid for all points in space, and ii) it recognizes the existence of toroidal moments. The electromagnetic field due to alternating poloidal currents in a toroidal solenoid is evaluated exactly via ...
Exam 1
Exam 1

magnetic moment and magnetization - Andrew.cmu.edu
magnetic moment and magnetization - Andrew.cmu.edu

Many-body interactions in the quantum well under strong optical
Many-body interactions in the quantum well under strong optical

Electric Fields and Conductors
Electric Fields and Conductors

Maxwell and Special Relativity - Physics Department, Princeton
Maxwell and Special Relativity - Physics Department, Princeton

... the transformation of the magnetic field. In particular, if B = 0 while E were due to a single electric charge at rest (in the unprimed frame), then magnetic Galilean relativity predicts that the moving charge/observer would consider the magnetic field B to be zero, whereas it is nonzero according to ...
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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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