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Frobenius-Perron Resonances for Maps with a Mixed Phase Space
Frobenius-Perron Resonances for Maps with a Mixed Phase Space

... recently attracted attention, e.g. in a superanalytic approach to universal fluctuations in quantum (quasi-) energy spectra which originated from the physics of disordered systems. In that approach the Frobenius-Perron resonances constitute a link between classical and quantum chaos [5,6]. There is ...
Polaronic exciton in a parabolic quantum dot
Polaronic exciton in a parabolic quantum dot

Chapter 6 Particle Spin and the Stern
Chapter 6 Particle Spin and the Stern

Non-Gaussianity of quantum states: an experimental test on single
Non-Gaussianity of quantum states: an experimental test on single

QUANTUM GROUPS AND DIFFERENTIAL FORMS Contents 1
QUANTUM GROUPS AND DIFFERENTIAL FORMS Contents 1

... Furthermore, the bialgebra Mq is universal with respect to these properties. The coaction of Mq on the generators of Ω(Aq ) is given by equation (1.1). In principle, the theorem can be verified directly from the definitions. But that is not a good approach because it does not tell us how to construc ...
Blueshift of the surface plasmon resonance in silver nanoparticles
Blueshift of the surface plasmon resonance in silver nanoparticles

... diameters ranging from 26 down to 3.5 nm. Our results also confirm very recent experiments made with Ag nanoparticles on different substrates using different STEM operating conditions [10], thereby strengthening the interpretation that the blueshift is predominantly associated with the tight confine ...
Quantized conductance for neutral matter
Quantized conductance for neutral matter

Past Research
Past Research

... of deformations (but under strong restrictions on G), and [48], generalizing results of Ram and Shepler [32] on graded Hecke algebras to a twisted case. My (then) Ph.D. student Shakalli generalized in [33] some of the ideas in [47] to deformations of Sq (V )#G, where Sq (V ) is a quantum symmetric a ...


The Physical World as a Virtual Reality
The Physical World as a Virtual Reality

Entanglement Theory and the Second Law of Thermodynamics
Entanglement Theory and the Second Law of Thermodynamics

... Indeed, our result suggests that such an irreversibility could have its roots on the assymmetry of operations that can be locally implemented without any entanglement (LOCC) and the operations that do not generate any entanglement. Moreover, it also represents a conterargument to linking irreversibi ...
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... • MgB2 ...
RLE_PR_140_02_01s
RLE_PR_140_02_01s

Effective electron-atom interactions and virial coefficients in alkali
Effective electron-atom interactions and virial coefficients in alkali

Landau levels in graphene
Landau levels in graphene

... However, in quantum mechanics wave function ψ describing the electron in magnetic field cannot be eigenfunction of X1 and X2 at the same time. Therefore the center of the orbit cannot be determined with arbitrary precision even in principle. Classical circular orbits can be (to certain precision) ob ...
Many-particle interference beyond many-boson and many
Many-particle interference beyond many-boson and many

... The symmetrization postulate enforces the (anti)symmetrization of the bosonic (fermionic) many-particle wavefunction [1] and thereby severely restricts the set of accessible states for indistinguishable particles. When one postulates that each microscopic state is populated with equal probability [2 ...
history of quantum computing
history of quantum computing

Dynamical Theories of Brownian Motion
Dynamical Theories of Brownian Motion

ElasticScattering - NUCLEAR REACTIONS VIDEO Project
ElasticScattering - NUCLEAR REACTIONS VIDEO Project

FlerasLectures - University of Oklahoma
FlerasLectures - University of Oklahoma

... foundation of the field. The components of the nucleus were subsequently discovered in 1919 (the proton) and 1932 (the neutron). In the 1920s the field of quantum physics was developed to explain the structure of the atom. The binding of the nucleus could not be understood by the physical laws known ...
Weak-Equivalence Principle Violation and Mass Change
Weak-Equivalence Principle Violation and Mass Change

... a gravitational mass increase is predicted by the same amount. This leads to a deviation of the Weak-Equivalence-Principle for both electrons and positrons at an order of 2.4%. This is a factor of 5 below the only measurement by Witteborn et al [2] and should be detectable with modern means. For exa ...
Bending Dynamics of Acetylene: New Modes Born in Bifurcations of
Bending Dynamics of Acetylene: New Modes Born in Bifurcations of

... its analytic and scalable character; in the next section, we present details of implementation. The Hamiltonian in (18) is a nonintegrable system. In general, the dynamics of such a system can only be understood by numerical integration of Hamilton’s equations and subsequent analysis, e.g., with sec ...
Quantum Error Correction - Quantum Theory Group at CMU
Quantum Error Correction - Quantum Theory Group at CMU

boltzmann`s entropy and time`s arrow
boltzmann`s entropy and time`s arrow

Basics of Particle Physics - The University of Oklahoma
Basics of Particle Physics - The University of Oklahoma

... foundation of the field. The components of the nucleus were subsequently discovered in 1919 (the proton) and 1932 (the neutron). In the 1920s the field of quantum physics was developed to explain the structure of the atom. The binding of the nucleus could not be understood by the physical laws known ...
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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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