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PH504lec1011-6-capa
PH504lec1011-6-capa

Thomson`s Theorem of electrostatics: Its Applications
Thomson`s Theorem of electrostatics: Its Applications

Momentum Transfer to a Free Floating Double Slit
Momentum Transfer to a Free Floating Double Slit

... Quantum mechanics poses a major challenge to our intuition which is trained in the macrocosm to the laws of classical physics. Among all the quantum phenomena, the double-slit interference is ‘‘a phenomenon which is impossible (. . .) to explain in any classical way, and which has in it the heart of ...
Wednesday, Feb. 1, 2012
Wednesday, Feb. 1, 2012

See also "SPINNING MAGNETIC FIELDS"
See also "SPINNING MAGNETIC FIELDS"

`Bound` states of an electron in the far
`Bound` states of an electron in the far

... with a (2l + 1)-fold degeneracy resulting from the spherical symmetry. A quantum condition similar to equation (25) would then arise from the radial equation with E = 0. ...
Line shapes - Center for Ultracold Atoms
Line shapes - Center for Ultracold Atoms

... The SOF technique is based on an interference between the excitations produced at two separated fields - thus it is sensitive to the phase difference (coherence) of the oscillating fields. The method is most easily understood by consideration of the classical spin undergoing magnetic resonance in SO ...
Spin-current and other unusual phases in magnetized triangular lattice antiferromagnets
Spin-current and other unusual phases in magnetized triangular lattice antiferromagnets

... 1#4, 1#2, and 3#4, and the overall shape of the magnetization curve is not in agreement with experiments. A closely related physical picture is obtained by describing the magnetized triplets by hard-core bosons [15]. Then the repulsion may favor charge-density wave states that are among the known in ...
Electromagnetic induction (16-19)
Electromagnetic induction (16-19)

Anisotropy and Magnetization Reversal
Anisotropy and Magnetization Reversal

Steady-state quantum interference in resonance
Steady-state quantum interference in resonance

... will occur in the total fluorescence, but only in certain polarisations. On the other hand, if the excited states are Rydberg states with different principal quantum numbers, it is possible for their J and mJ values to be equal, thereby allowing quantum interference to affect the total fluorescence. ...
Kondo, Fano and Dicke effects in side quantum dots
Kondo, Fano and Dicke effects in side quantum dots

... We have studied the transport through a side-coupled double quantum-dot molecule using the finite-U slave boson mean field approach. The transmission spectrum shows a structure with two antiresonances localized at the bonding and antibonding renormalized energies of the quantum-dot molecule, and one ...
Antenne_verslag_eng
Antenne_verslag_eng

Stage 6 HSC Biology Advanced DiagnosticTests
Stage 6 HSC Biology Advanced DiagnosticTests

NMR_1
NMR_1

... a characteristic frequency, To observe resonance, all we have to do is irradiate them with electromagnetic radiation of the appropriate frequency. •It’s easy to understand that different nucleus “type” will give different NMR signal. (remember v =w/2= B0/2 ? Thus, different  cause different v !! ...
Part II
Part II

Electric Field
Electric Field

Quantum critical point and spin fluctuations in the lower
Quantum critical point and spin fluctuations in the lower

... Fe2+ ions can dramatically alter the physical and chemical properties of (Mg,Fe)O in the deep mantle, thereby changing our understanding of the Earth’s deep interior. To establish a fundamental understanding of the ground electronic state of iron, the electronic and magnetic states of Fe2+ in (Mg0.7 ...
Quantum Physics Lecture Notes
Quantum Physics Lecture Notes

Calculation of Magnetic Field Disturbance Produced by Electric
Calculation of Magnetic Field Disturbance Produced by Electric

Motion of charged particles in magnetic fields created by symmetric
Motion of charged particles in magnetic fields created by symmetric

... ∂φ . r2 It is clear that this vector field has the symmetries S1 = ∂z (translation) and S2 = ∂φ (rotation), and hence the integral curves of BR are circles around the z-axis. We are interested in the motion of a unit-charge, unit-mass particle subjected to the magnetic field BR . The interest of thi ...
Chapter 24 – Capacitance and Dielectrics
Chapter 24 – Capacitance and Dielectrics

American Association Of Physics Teachers Meeting January 1999  Anaheim, CA supporting
American Association Of Physics Teachers Meeting January 1999 Anaheim, CA supporting

Electrostatics I
Electrostatics I

Physics of wave packets
Physics of wave packets

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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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