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Stochastic mechanism of excitation of molecules that interact with
Stochastic mechanism of excitation of molecules that interact with

Monte Carlo Simulations of Quantum Spin Models - cond
Monte Carlo Simulations of Quantum Spin Models - cond

CHEM-UA 127: Advanced General Chemistry I
CHEM-UA 127: Advanced General Chemistry I

... If we could neglect the electron-nuclear interaction, then the wave function would be a simple product Ψ(x, R) = ψelec (x)ψnucl (R). However, we cannot neglect this term, but it might still be possible to write the wave function as a product. We note, first, that most nuclei are 3-4 orders of magnit ...
www.osa-opn.org 36 | OPN Optics & Photonics News Illustration by Phil Saunders/ spacechannel.org
www.osa-opn.org 36 | OPN Optics & Photonics News Illustration by Phil Saunders/ spacechannel.org

... quantum information processing protocols. In the presence of photon-pair entanglement, each of the constituent single photons becomes a statistical mixture of the relevant spectral and spatial modes, so that the detection of one of the photons heralds (i.e., announces the presence of) a single photo ...
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... be compiled into an optimal solution, a multivariate function of all parameters, known as the I − f unction of that family. This is the object of interest in quantum mirror symmetry. For one-parameter families, the Dwork-Griffiths method provides a method to compute the (one) Picard-Fuchs equation. ...
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Document

... system, the [distant] second system may be left in states with two different [types of] wavefunctions.” • 1935 Schrödinger’s entanglement = nonseparability. “Maximal knowledge of a total system does not necessarily include total knowledge of all its parts, not even when these are fully separated fro ...
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PDF

... the entangled qubits from a singlet state into two L-km-long standard telecommunication fibers. The photons emerging from the fibers are then loaded into trapped-atom quantum memories [3]. These memories store the photon-polarization qubits in long-lived hyperfine levels. Because it is compatible with ...
Musical Modulation by Symmetries
Musical Modulation by Symmetries

Ch27 The Electric Field
Ch27 The Electric Field

...  Use the concept of superposition to find the  Translate the sum into an ...
Realization of Bose-Einstein Condensation in dilute gases
Realization of Bose-Einstein Condensation in dilute gases

Mathematical Foundations of Quantum Physics
Mathematical Foundations of Quantum Physics

... electrodynamics by Feynman, Dyson, Schwinger, and Tomonaga during the 1940s. Quantum electrodynamics is a quantum theory of electrons, positrons, and the electromagnetic field, and served as a role model for subsequent quantum field theories. The theory of quantum chromodynamics was formulated begin ...
From quantum cloning to quantum key distribution with
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Daqоq al-Kal¥m: A Basis for an Islamic Philosophy of Science
Daqоq al-Kal¥m: A Basis for an Islamic Philosophy of Science

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Information in statistical physics

... PPauli operators σ̂x, σ̂y , σ̂z , which are characterized by the algebra σ̂iσ̂j = i k εijk σ̂k ; for a particle on a line, the algebra is generated by the position and momentum operators x̂ and p̂ in the Hilbert space of wavefunctions, with [x̂, p̂] = i~. The specific features of quantum physics, co ...
Graduate Course Descriptions - UC Berkeley Physics
Graduate Course Descriptions - UC Berkeley Physics

Passive Dynamics and Particle Systems COS 426
Passive Dynamics and Particle Systems COS 426

... 4. V = rotate A around N by t1 5. V = rotate V around VxN by acos(t2) ...
Two-Level Atom at Finite Temperature
Two-Level Atom at Finite Temperature

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Self-dual Quantum Electrodynamics as Boundary State of the three

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A THEORY OF DEDUCTION FOR QUANTUM MECHANICS Abstract

... If we now want to treat individual YES-NO measurements, we have to introduce frequenci~s and if we are to stay within quantum formalism the frequencies have to be introduced on an infinite number of trials, i.e . the frequencies have to be ideal. Let N + = N Jp,N) be the number of successes in the f ...
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... Finally, we can also form direct product bases using a discrete basis for one space and a continuous basis for the other. Note, that by unitary transformation in the product space it is generally possible to produce bases which are not the direct products of bases in the factor spaces (i.e., ONB’s f ...
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The Universal Electrodynamic Force

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Characterizing the Performance Effect of Trials and Rotations in

... A class of computational problems exist for which no polynomial-time algorithm running on a classical Turing Machine has yet been proposed. However, a number of these algorithms—with important practical implications—have been found to be efficiently solvable using a quantum computer. This is known a ...
Introductory quantum mechanics
Introductory quantum mechanics

... becomes fuzzy when it’s represented by its matter wave. We can no more tell for sure where it is exactly located.  Recall that in the case of conventional wave physics, |field amplitude|2 is proportional to the intensity of the wave). Now, what does |Y |2 physically mean? ...
Three measurement problems | SpringerLink
Three measurement problems | SpringerLink

A REPORT ON QUANTUM COMPUTING
A REPORT ON QUANTUM COMPUTING

... referred to as a 'qubit', exist in the classical 0 and 1 states, it can also be in a coherent superposition of both. When a qubit is in this state it can be thought of as existing in two universes, as a 0 in one universe and as a 1 in the other. An operation on such a qubit effectively acts on both ...
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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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