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Spontaneous Formation of Magnetic Moments and Dephasing in Two-Dimensional Disordered Systems
Spontaneous Formation of Magnetic Moments and Dephasing in Two-Dimensional Disordered Systems

... temperature goes down the external degrees of freedom freeze out, so that coherence time will be infinite at zero temperature. For temperatures less than one Kelvin, the phonon’s contribution to dephasing becomes negligible and the main processes of dephasing are due to electron-electron interaction ...
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... spinons as originally suggested, but that these spinons are descendents of the 1D excitations of the chains formed by the strong J bonds, and not characteristic of any exotic 2D state. A popular argument against this notion has been that the peak energy has substantial dispersion in the direction tr ...
Studies in Quantum Information Theory
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... be, and Shivaji did too. And for that I am truly grateful. A huge thanks goes to Chiara and Herman, who were supportive during their respective tenures as Director of Graduate Studies, and I should also mention Laurel Lerner as being a huge help every step of the way. I believe this truly is one of ...
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... One might be tempted to conclude from this that a phenomenological description is simply not possible beyond the delta function approximation. After all, if the underlying theory is known, one can always compute the corrections without any approximation, and it might be argued that the inconsistenci ...
Complexity Science as Order-creation Science
Complexity Science as Order-creation Science

... How do the race probabilities emerge from the interference of the fine-grained structure? Gell-Mann says that when we “sum over” all of the detailed factors left out—not the tips of the noses of the few horses in, say, the fourth race—the interference effects average out at approximately zero. Hence ...
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Macroscopic quantum effects based on Kerr nonlinearities
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... These notes are organized as follows. We introduce in section 2 the classical dynamical systems we will focus on (mostly geodesic flows and maps on the 2dimensional torus), mentioning their degree of “chaos”. We also sketch the quantization procedures leading to quantum Hamiltonians or propagators, ...
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... Quantum description of the field propagating in a Kerr medium, which will be the subject of our concern in this chapter, reveals a number of interesting features that we are going to address here. Nonclassical effects associated with the anharmonic oscillator model have been discussed in many papers ...
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... effect, this leads to quantization of the transmitted charge, and is of metrological use [10]. Devices of this type are called ‘single-electron turnstiles’. Charge pumping is achieved by varying certain parameters of the system Hamiltonian periodically with time. When the change is carried out slowl ...
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... In the preceding section, we showed that the numerical simulation of the truncated system appears to validate the LSB process. For a large value of N, this result is still an approximation. However, the system can be modeled exactly for very small values of N. In particular, if we choose N ¼2, there ...
Interacting Quantum Observables: Categorical Algebra and
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... Previous work established the remarkable fact that every algebra of this kind on a finite dimensional Hilbert space arises as pair of copying and erasing operations for some orthonormal basis [27, 28]. Since these algebras correspond precisely to nondegenerate quantum observables, we refer to them a ...
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... This operator (”R-matrix “) captures contributions of a single vertex to the partition function. Consider an (N + 1)-fold tensor product V0 ⊗ V1 ⊗ · · · ⊗ VN (Vi = V ) and let Rij be the operator acting on the Vi ⊗ Vj component of this product as R and as identity on any other Vl . ...
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... Dirac fermions have energies EN ¼ sgn(N)vF(2eB:|N|)1/2, where sgn is the sign function, N is the LL index (positive for electrons and negative for holes), vF is the Fermi velocity, e is the elemental charge and : is the Plank’s constant h divided by 2p. The zeroth LL at E0 ¼ 0 is equally shared betw ...
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... the physics, though the transparency of the model may be greater with one or the other, depending of the nature of the problem. For low atomic densities the atomic basis is convenient (see for example [27]), whereas at high densities where collisions play a dominate role the molecular basis is more ...
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... define charge-number states with |n where n is a number of excess Cooper pairs in the right electrode. Because of the conservation of the total charge, the left electrode has (−n) excess Cooper pairs. The chargenumber states are the ground state of the two superconductors with such a particular char ...
The Quantum Hall Effect: Novel Excitations and Broken Symmetries
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Path Integral studies of quantum systems at finite temperatures Sergei Dmitrievich Ivanov
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... wavelength becomes comparable with the average distance between the particles in the system, i.e., the quantum delocalization effects become important. Usually it happens in either dense systems or at low temperatures. For electrons, due to their small mass, even room temperature is low, that is why ...
Anti Heisenberg. The end of Heisenberg`s uncertainty principle.
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... Copyright © 2016 by Ilija Barukčić, Jever, Germany. ...
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Interpretations of quantum mechanics

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