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Laser-induced fluorescence measurements of argon ion velocities
Laser-induced fluorescence measurements of argon ion velocities

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Thessa_pres

Electric Fields and Solvation in Microscopic Liquids
Electric Fields and Solvation in Microscopic Liquids

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Superconducting Qubits: A Short Review

... temperatures where the typical energy kT of thermal fluctuations is much less that the energy quantum ~ω 01 associated with the transition between the states |qubit=0> and |qubit=1>. For reasons which will become clear in subsequent sections, this frequency for superconducting qubits is in the 5-20 ...
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FIRST MIDTERM - REVIEW PROBLEMS
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... Calculate the magnitude of the electric field 4.00 × 10 - 12 m away from a proton, which has a positive charge identical in magnitude to the electron. Calculate the term in x 6 for the binomial expansion of (1 - x 2) - 9/2. Calculate the electric force between two protons a distance 2.00 × 10 - 13 m ...
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Universal emergence of the one-third plateau
Universal emergence of the one-third plateau

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Generace, ztráty a diagnostika ubíhajících elektron˚uv

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Superconducting Qubits: A Short Review

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Chapter 6: Maxwell`s Equations for Time-Varying Fields

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... I would like to express my thanks to Prof. Weimin Chen and Prof. Irina Buyanova for giving me the opportunity to work in their group. I want to thank you for all invaluable, stimulating discussions and for always finding some light in the darkest maze of data. I am grateful to Arne Eklund and Roger ...
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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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