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Quantum Techniques for Stochastic Mechanics
Quantum Techniques for Stochastic Mechanics

... stochastic Petri nets, they describe how collections of things of different kinds randomly interact and turn into other things. In Section 18 we consider a simple example of the deficiency zero theorem taken from chemistry: a diatomic gas. In Section 19 we apply the Anderson– Craciun–Kurtz theorem t ...
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... photon states are well explained by the Tavis-Cummings model over a wide range of detunings. On resonance we observe all but two eigenstates to be dark states, which do not couple to the cavity field. The bright states on the other hand are an equal superposition of a cavity photon and a multi-qubit ...
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... The Mollow Absorption Spectrum of a Neutral QD . . . . . . . . . . 37 Band Structure and Energy Level Diagram of The Trion State . . . . 44 Trion Mollow Absorption Spectrum . . . . . . . . . . . . . . . . . . . 46 Signatures of Heavy-light Hole Mixing . . . . . . . . . . . . . . . . . 54 Signature o ...
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... the gap for all the high-symmetry points and lines for the 138 space groups without inversion symmetry. A complete list of all the cases is lengthy and is summarized in the tables in the Supplementary Materials. In Fig. 4, we summarize possible patterns for positions where the gap closes in k space ...
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... the gap for all the high-symmetry points and lines for the 138 space groups without inversion symmetry. A complete list of all the cases is lengthy and is summarized in the tables in the Supplementary Materials. In Fig. 4, we summarize possible patterns for positions where the gap closes in k space ...
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... In this work we study a Bose–Einstein condensate of 87 Rb under the effects of an oscillatory excitation. The condensate is produced through forced evaporative cooling by radio–frequency in a harmonic magnetic trap. The excitation is generated by an oscillatory quadrupole field superimposed on the t ...
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... ISBN 0444869387 Bbc- Investigación 53.01 FOL http://encore.ehu.es/iii/encore/record/C__Rb1005283 Of all the developments in twentieth century physics, none has given rise to more heated debates than the changes in our understanding of science precipitated by the ``quantum revolution''. In this revol ...
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... I Multivariate differential and integral calculus in cartesian and non-cartesian (cylindrical and spherical) coordinate systems at the level of Ph1abc. I Vectors and vector operations at the level of Ph1abc. I Methods for solving first- and second-order linear ordinary differential equations at the ...
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... of the correlated final spin system. Explicit spin-dependent interactions are neglected and electron exchange only is taken into account. It is shown that the final spin system is completely characterized by a single spin correlation parameter depending on scattering angle and energy. Its numerical ...
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... at −h/2e2 (the value for a SLG QHE) with accompanying R12xx now displaying a resistance plateau (at h/4e2 ) rather than vanishing. The observation [Figs. 2(c) and 2(d)] that the quantized R12xy switch between SLG-like and BLG-like values when either the carrier type or the B field is reversed implie ...
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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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