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Introduction to Quantum Computing (2010) (e-book)
Introduction to Quantum Computing (2010) (e-book)

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... Organization of the Thesis The sequence of chapters can be divided into three blocks. • The first block contains the introductory chapters. In chapter 1 we illustrate the problem of the high-Tc superconductors making a parallelism between the Fermi Liquid theory, the BCS theory of superconductivity ...
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... The frontier between the classical and quantum worlds can be approached in one of two ways: from the top down or the bottom up. The top-down approach entails starting with an essentially classical variable (e.g. the flux in a superconducting loop, the charge on a small superconducting island or the ...
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... Dry air will break down and generate a spark if the electric field exceeds about 3 × 10 6 N C . How much charge could be packed onto a green pea (diameter 0.75 cm) before the pea spontaneously discharges? [Hint: Eqs. 16–4 work outside a sphere if r is measured from its center.] ...
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... by Osherson and Smith [5]. These authors considered the concepts Pet and Fish and their conjunction Pet-Fish, and observed that, while an exemplar such as Guppy was a very typical example of Pet-Fish, it was neither a very typical example of Pet nor of Fish. Therefore, the typicality of a specific e ...
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... We describe a ferromagnetic domain in a magnetic material by the Ising model using the language of statistical mechanics. By heuristic arguments we show that there is no spontaneous magnetization for the nearest-neighbour Ising model in one dimension and that there is spontaneous magnetization in tw ...
< 1 ... 45 46 47 48 49 50 51 52 53 ... 661 >

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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