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Frustrated Magnetism in Vanadium Oxides
Frustrated Magnetism in Vanadium Oxides

Effective lattice models for two-dimensional
Effective lattice models for two-dimensional

... of the monopoles. For N = 1, kµ = 0; the action for each monopole-anti-monopole pair is given by that of the vµ string connecting them ∼ G(0)R ∼ R/g. (ii) Large g The vµ and kµ fluctuations are less strongly coupled. We integrate out the n fluctuations in Sf (Eqn 4) by a ‘high-temperature’ expansion ...
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AN INDEX THEORY FOR QUANTUM DYNAMICAL SEMIGROUPS 1

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... Thermodynamics, has the generally accepted interpretation in the theory of gases that the entropy vanishes in the zero temperature limit. Schrödinger [1] had pointed out long ago that when two states contribute to the ground state of a many particle system that a finite constant term could appear i ...
Student Colloquium at WSU (Fall 2006) (ppt-format)
Student Colloquium at WSU (Fall 2006) (ppt-format)

... Hadronization in medium (i.e. during universe expansion) could be different because medium might affect the mechanism. ...
Rapid readout of a register of qubits using open loop... Joshua Combes , Aaron Denney , and Howard M. Wiseman
Rapid readout of a register of qubits using open loop... Joshua Combes , Aaron Denney , and Howard M. Wiseman

... measurement extracts information from a quantum system for a reasonably general measurement model. The starting point for our analysis is the quantum trajectory description of the measurement process. The physics behind the quantum trajectory description is as follows. Consider using an ancilla, e.g ...
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QM L-8 particle in

Two interacting spin particles - Dipartimento di Matematica e Fisica
Two interacting spin particles - Dipartimento di Matematica e Fisica

... eigenfunctions in this basis can be directly related to singleparticle operators, in particular, with the distribution of occupation numbers for single-particle states. The Hamiltonian matrix has a clear band structure, with the bandwidth b ranging from 1 at the corners up to b52l 11 in the middle. ...
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Transport through interacting quantum wires and nanotubes

... QGL action, coefficients from full model ...
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Calculation Algorithm for Finding the Mini

... with the possible exception that ...
Quantum Entanglement in Many-body Systems
Quantum Entanglement in Many-body Systems

... quantum entanglement. In this sense, quantum entanglement may be considered as an emergent phenomenon. Unfortunately, our understanding of quantum entanglement is still very limited. In fact, quantum entanglement has been quantified properly only for special cases, namely bipartite systems. Many-bod ...
Bringing Together Gravity and the Quanta
Bringing Together Gravity and the Quanta

Gravity as a fluid dynamic phenomenon in a superfluid
Gravity as a fluid dynamic phenomenon in a superfluid

arXiv:0905.2946v1 [cond-mat.str-el] 18 May 2009
arXiv:0905.2946v1 [cond-mat.str-el] 18 May 2009

Chapter 10.
Chapter 10.

... thinking” [Manin99]? “Quantum Computing” comprises theories, algorithms and techniques for exploiting the unique nature of quantum events to obtain computational advantages. Actually that is not the reason, the fact is that the quantum computer promises great future for computing: it significantly r ...
Algebraic Quantum Field Theory on Curved Spacetimes
Algebraic Quantum Field Theory on Curved Spacetimes

High Energy Physics (3HEP) - Physics
High Energy Physics (3HEP) - Physics

... electron. We write their four-momenta to describe the conservation of both energy and momentum: • e-(E0,0) → e-(Ek,-k)+ γ(ck,k) Where we have already made sure momentum is conserved by construction. In free space (e.g. not in a an electric field from which can do work on the electron): E0=mc2, Ek=(k ...
Spintronics and Quantum Dots for Quantum Computing and
Spintronics and Quantum Dots for Quantum Computing and

... a growing list of quantum tasks [9,10] such as cryptography, error correcting schemes, quantum teleportation, etc. that have indicated even more the desirability of experimental implementations of quantum computing. In a quantum computer each quantum bit (qubit) is allowed to be in any state of a qu ...
Power of one qumode for quantum computation Please share
Power of one qumode for quantum computation Please share

distribution functions in physics: fundamentals
distribution functions in physics: fundamentals

Quantum-well states and discontinuities in opto
Quantum-well states and discontinuities in opto

Lecture 8: The fractional quantum Hall effect The fractional quantum
Lecture 8: The fractional quantum Hall effect The fractional quantum

Book Review: It Must Be Beautiful: Great Equations of Modern
Book Review: It Must Be Beautiful: Great Equations of Modern

... equation is E = ω , where ω is the angular frequency (frequency measured in radians per second), and  is a conversion constant (rationalized Planck’s constant). This equation has the same flaw; it deals with only one component of a vector. The accompanying equation for the other three components w ...
Randomness in (Quantum) Information Processing
Randomness in (Quantum) Information Processing

Gate-defined quantum confinement in suspended bilayer graphene
Gate-defined quantum confinement in suspended bilayer graphene

... externally applied fields. At B = 0, breaking layer inversion symmetry opens an energy gap tunable up to 250 meV with an external perpendicular electric field E (refs 19–25) that can be used for confinement. In devices with low disorder and at high magnetic fields, gapped states emerge from Coulomb- ...
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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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