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Generation of arbitrary Dicke states in spinor Bose±Einstein
Generation of arbitrary Dicke states in spinor Bose±Einstein

... squeezed states with arbitrary prescribed value of hJ^z i ˆ m0 and arbitrary Dicke states, we propose to use instead the following method: ®rst, a coupling pulse of appropriate strength is applied to the ground state jj; ji, creating an initial CSS with hJ^z i ˆ m0 . Assume without loss of generalit ...
pdf - at www.arxiv.org.
pdf - at www.arxiv.org.

Entropy is in Flux - James Franck Institute
Entropy is in Flux - James Franck Institute

No. 1-fn.p65 - Department of Atomic Energy
No. 1-fn.p65 - Department of Atomic Energy

Classical properties of quantum scattering
Classical properties of quantum scattering

... which have become a very convenient form to represent the scattering waves. Researchers who followed Lord Rayleigh’s analysis introduced an estimation of the effectiveness of scattering and the interaction between the incident plane wave and the perturber (which later were associated with scattering ...
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... to the cuprate superconductors Colloquium article in Reviews of Modern Physics 75, 913 (2003) ...
Quantum interference in the field ionization of Rydberg atoms
Quantum interference in the field ionization of Rydberg atoms

... Because the valence electron in a Rydberg atom is only weakly bound to the core, its energy levels are easily shifted by the Stark effect with modest electric fields. The resulting rich behavior of Rydberg atoms in electric fields has been exploited for a wide range of experiments. Recently, Rydberg ...
Algebraic Study on the Quantum Calogero Model
Algebraic Study on the Quantum Calogero Model

... China, August 19- 2-1 , 1996, ed. l\1.-L. Ge, Y. Saint-Au bin and L. Vinet (Springer- \"erlag). ...
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slides

Constructor theory of information - Proceedings of the Royal Society A
Constructor theory of information - Proceedings of the Royal Society A

... medium of the receiver to another state x or y respectively, thus making a copy of the message while leaving the original message unchanged. But, this does not, in fact, distinguish message x from message y unless the resulting receiver states x and y are themselves distinguishable. Thus, (1.1), con ...
Classical Mechanics - UC Riverside (Math)
Classical Mechanics - UC Riverside (Math)

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... superfluidity (a version of the BCS theory that can be found e.g. in [34]). The notion of a representation of the CCR and CAR gives a convenient framework to describe Bogolubov transformations and their unitary implementations. Analysis of Bogolubov transformations becomes especially interesting in t ...
Compatibility of Quark and Resonant Picture Excited Baryon
Compatibility of Quark and Resonant Picture Excited Baryon

Flux quanta, magnetic field lines, merging
Flux quanta, magnetic field lines, merging

... is quantised. One easily realises that in a magnetic mirror geometry where the particles oscillate between the mirror points the parallel energy of the electron bounce motion pk2 /2me ≡ b = h̄ωb (s + 12 ) would also be quantised with bounce frequency ωb  ωce and parallel quantum number s = 0,1,2,3 ...
Thermodynamics of the high temperature Quark-Gluon - IPhT
Thermodynamics of the high temperature Quark-Gluon - IPhT

... These are at present the unique tools allowing a detailed study of the transition region where various interesting phenomena are taking place, such as colour deconfinement or chiral symmetry restoration. In these lectures, we shall not consider this transition region, but focus rather on the high te ...
Naturalness via scale invariance and non-trivial UV fixed points in a 4d O(N) scalar field model in the large-N limit
Naturalness via scale invariance and non-trivial UV fixed points in a 4d O(N) scalar field model in the large-N limit

... actions when regulators are removed. It is the latter that is physically observable and defines the theory. Such a scenario is not amenable to analysis via the loop expansion, traditional perturbation theory or a weak field expansion in powers of the scalar field. In particular, we give up perturba ...
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THE WIGHTMAN AXIOMS AND THE MASS GAP FOR STRONG

Introduction - Princeton University Press
Introduction - Princeton University Press

Optical Properties of Semiconductor Nanostructures in Magnetic Field DISSERTATION
Optical Properties of Semiconductor Nanostructures in Magnetic Field DISSERTATION

... increasing and these structures are nowadays considered to be even more perspective for future applications e.g. for quantum computing. This is one of the reasons why after such a long time the amount of research performed on this field does not decrease but grows further. The scientific interest an ...
Could light harvesting complexes exhibit non
Could light harvesting complexes exhibit non

An overview of factors influencing the colloid/particle favoured
An overview of factors influencing the colloid/particle favoured

On Complex Structures in Physics
On Complex Structures in Physics

... solution of the problem of di raction of waves on a half-plane [20]1. Roger Penrose, in his twistor theory, put forward convincing arguments in favor of the relevance of holomorphic structures for fundamental physics [11, 13]. His methods and ideas have been successfully used in a variety of mathema ...
acta physica slovaca vol. 50 No. 1, 1 – 198 February 2000
acta physica slovaca vol. 50 No. 1, 1 – 198 February 2000

... We present in this work a straightforward, and a “very natural” theoretical extension of traditional (linear) quantum mechanics (QM), providing a general framework of several physical theories. It contains QM itself, its (almost all up to now published) nonlinear modifications and extensions, and al ...
PowerPoint Notes
PowerPoint Notes

... • Calculate the de Broglie wavelength of matter waves. • Distinguish between classical ideas of measurement and Heisenberg’s uncertainty principle. • Describe the quantum-mechanical picture of the atom, including the electron cloud and probability waves. ...
Automated Design of Quantum Circuits - vlsicad page
Automated Design of Quantum Circuits - vlsicad page

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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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