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A Short Course on Topological Insulators
A Short Course on Topological Insulators

Lectures CP violation
Lectures CP violation

Dynamics of the two-spin spin-boson model with a
Dynamics of the two-spin spin-boson model with a

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Patterns of Electro-magnetic Response in Topological Semi

Contents
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... invariance – and represent the interaction under study. If the symmetry group is non-commutative, it is referred to as nonAbelian, like in the Yang–Mills theory that is briefly addressed in the appendix. When the theory is quantized, the quanta of the gauge fields are called gauge bosons. Quantum e ...
Compass models: Theory and physical motivations
Compass models: Theory and physical motivations

... such as vacancy centers, and cold atomic gases. The fundamental interdependence between internal (spin, orbital, or other) and external (i.e., spatial) degrees of freedom which underlies compass models generally leads to very rich behaviors, including the frustration of (semi-)classical ordered stat ...
Introduction to Lattice Field Theory
Introduction to Lattice Field Theory

... For a new formulation of quantum mechanics we have a trivial algorithm for computing the energy. It exploits the simple fact that given a randomly chosen unit vector |φi, the matrix element hφ| T n |φi tends to λn0 as n → ∞. 1. Choose a source. At one time slice construct a random linear combination ...
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Two-gluon rapidity correlations of strong colour

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Algebraic Topology Foundations of Supersymmetry and Symmetry

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Axial gravity, massless fermions and trace anomalies

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Ultracold atoms in optical lattices with long- PhD Thesis

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Landau`s Fermi Liquid Theory

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... of work that followed, it became clear that a useful framework for under standing this situation is Atiyahs axiomatic description of a topological quantum eld theory, or TQFT. On the other hand, at about the same time as Jones initial discov ery, Ashtekar discovered a reformulation of general relati ...
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- Philsci-Archive

... What I am doing is using history as a guide to a tentative clarification of some unclear aspects of the theory. Since I am not taking into account more recent contributions, a work that goes back to the early fifties of last century and before might seem dated. Here I must distinguish between the a ...
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The Pokorski Group Story III. 1. The Beginnings Among those who

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2010 - Universiteit Utrecht

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AdS/CFT Course Notes - Johns Hopkins University

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Strongly correlated quantum physics with cold atoms - Max

... while, surprisingly, the initial solid order is preserved. This memory effect engineers the elusive supersolid state as a quantum superposition between superflow and solidity. We propose that the same principle could be applied to create other exotic forms of excited quantum matter – thus stimulating ...
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Efimov Trimers under Strong Confinement

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Chapter One : The Story of Magnetic Monopoles 0

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The Heisenberg antiferromagnet on the square

< 1 2 3 4 5 6 7 ... 120 >

Quantum chromodynamics

In theoretical physics, quantum chromodynamics (QCD) is the theory of strong interactions, a fundamental force describing the interactions between quarks and gluons which make up hadrons such as the proton, neutron and pion. QCD is a type of quantum field theory called a non-abelian gauge theory with symmetry group SU(3). The QCD analog of electric charge is a property called color. Gluons are the force carrier of the theory, like photons are for the electromagnetic force in quantum electrodynamics. The theory is an important part of the Standard Model of particle physics. A huge body of experimental evidence for QCD has been gathered over the years.QCD enjoys two peculiar properties:Confinement, which means that the force between quarks does not diminish as they are separated. Because of this, when you do separate a quark from other quarks, the energy in the gluon field is enough to create another quark pair; they are thus forever bound into hadrons such as the proton and the neutron or the pion and kaon. Although analytically unproven, confinement is widely believed to be true because it explains the consistent failure of free quark searches, and it is easy to demonstrate in lattice QCD.Asymptotic freedom, which means that in very high-energy reactions, quarks and gluons interact very weakly creating a quark–gluon plasma. This prediction of QCD was first discovered in the early 1970s by David Politzer and by Frank Wilczek and David Gross. For this work they were awarded the 2004 Nobel Prize in Physics.The phase transition temperature between these two properties has been measured by the ALICE experiment to be well above 160 MeV. Below this temperature, confinement is dominant, while above it, asymptotic freedom becomes dominant.
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