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The classical and quantum mechanics of a particle on a knot.
The classical and quantum mechanics of a particle on a knot.

... arise when we make a transition to quantum mechanics. In particular, the fact that the conjugate operators pθ and θ do not commute requires us to perform an operator-ordering of the classical Hamiltonian. The above analysis shows that while toroidal coordinates are ideally suited to consider the mot ...
Electric field dependence of magnetic properties
Electric field dependence of magnetic properties

... been hampered by a strong dependence on such aspects as the choice of the gauge origin, the choice of the basis set, and the description of electron correlation. In this work we study the electric field dependence of magnetic properties. The problems encountered in the calculation of magnetic proper ...
E d
E d

... A simple case is a system consisting of only two point charges + e and - e at a distance a. Such a system is called a (physical) electric dipole, its moment is equal to ea, the vector a pointing from the negative to the positive charge. Under the influence of the external electrical field, the posit ...
Are pulsars born with a hidden magnetic field? Alejandro Torres-Forné
Are pulsars born with a hidden magnetic field? Alejandro Torres-Forné

... The boundary between the unmagnetized material falling back and the force-free magnetosphere, i.e. the magnetopause, can be easily compressed at long distances (r & 108 cm ) due to the large difference of the pressure of the infalling material with respect to the magnetic pressure. The dynamical eff ...
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79, 245424 (2009)

Magnetism
Magnetism

... • Bring a magnet to an electrically charged object and nothing happens. No forces. • Bring a magnet near some metals (Co, Fe, Ni …) and it will be attracted to the magnet. – The metal will be attracted to both the N and S ...
The principle of relativity and the De Broglie relation - Loreto
The principle of relativity and the De Broglie relation - Loreto

Quantum Concepts for Chemistry
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Lecture Notes 14: Electromagnetic Radiation from An Arbitrary Source, Radiation Reaction on a Moving Point Charge

... bubble) – the latter of which very definitely can propagate / create sound precisely because sound waves are longitudinal, not transverse waves!! Now think about the electron – for EM radiation fields, electric dipole / quadrupole / etc. higher EM moments break the rotational invariance / rotational ...
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... charges of the opposite sign, thus making the system neutral. More precisely, we have to neutralize locally, so that the positive charge density should balance the negative charge density. Now let us add a test charge Q which make slight imbalance. We are interested to know what would be the electri ...
Excitation of an Atomic Electron to a Coherent Superposition of
Excitation of an Atomic Electron to a Coherent Superposition of

... quantum state distribution of our atomic cat state. This technique consists of ramping on a dc electric field which ionizes the population from different Rydberg states at different times as each state’s ionization potential is reached during the ramp. The ions are collected with an electron multipl ...
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... The modern era of superconducting quantum computation began in 2002. That year, the group of Siyuan Han at the University of Kansas and the group of John Martinis, then at NIST Boulder and currently at UC Santa Barbara, independently showed that long-lived quantum states in a current-biassed JJ can ...
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An Introduction to Quantum Computation

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Effect of MnO2 doping on the dielectric properties of barium titanate

Lecture 6: Maxwell`s Equations
Lecture 6: Maxwell`s Equations

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... rotation sense as the LHM or in the opposite sense. The frequency of an incident LG beam whose wave-front is screwing as the LHM is downshifted to ω ′ = ω − (σ + l)Ω, whereas a LG beam of the opposite sense is upshifted to ω ′ = ω −(σ−l)Ω. Unexpectedly, the rotational frequency shift in LHMs is unre ...
Maxwell`s equations
Maxwell`s equations

Lecture 6: Maxwell´s Equations
Lecture 6: Maxwell´s Equations

... They relate the electromagnetic field to the properties of the material, in which the field exists. Together with the Maxwell’s equations, the constitutive relations completely describe the electromagnetic field. Even the EM fields in a nonlinear media can be described through a nonlinearity existin ...
Lecture 6: Maxwell`s Equations
Lecture 6: Maxwell`s Equations

ppt - Harvard Condensed Matter Theory group
ppt - Harvard Condensed Matter Theory group

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Physics - New Horizon School

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Magnetic polyoxometalates: from molecular magnetism to molecular spintronics and quantum computingw

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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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