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Short Answers - rossnazirullah
Short Answers - rossnazirullah

Physics Unit1 QuestionBank
Physics Unit1 QuestionBank

... Physical quantities which do not depend upon any other quantity for their measurement are ___________ (a) derived quantity (b) fundamental quantity (c) ystem of units (d) none ...
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Manifestations of Berry`s phase in molecules and condensed matter
Manifestations of Berry`s phase in molecules and condensed matter

... the curvature in general does not vanish, and one gets non-trivial Berry’s phases even with simply connected ξ-domains. In this case the Berry’s phase γ can take any value, not just 0 or π. 2.4. The paradigm: the Aharonov–Bohm effect We illustrate the physical implications of the above mathematics f ...
Studies of Highly Polar Atomic and Molecular Systems: Quantum Dynamics Investigations
Studies of Highly Polar Atomic and Molecular Systems: Quantum Dynamics Investigations

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An optically detected cyclotron resonance study of bulk GaAs

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Quantum path-integral study of the phase diagram and isotope

... of neon is thus interesting because allows us to quantify systematic errors of treating the neon atoms as particles moving classically in the PES. However, we stress that these quantum corrections do not represent any kind of measurable property, i.e., they can not be directly compared to experiment ...
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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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