'Renormalization group' diaporamas de présentation

Density Matrix Renormalization Group DMRG

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Roberto Casalbuoni Department of Physics and INFN - Florence

QCD at very high density. Roberto Casalbuoni Department of Physics and INFN - Florence. http://theory.fi.infn.it/casalbuoni/ barcellona.pdf casalbuoni@fi.infn.it. Perugia, January 22-23, 2007. Summary. Introduction and basics in Superconductivity Effective theory BCS theory

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M ultiscale E ntanglement R enormalization A nsatz

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Holographic Renormalization Group with Gravitational Chern-Simons Term

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Heat Conduction in One-Dimensional Systems : molecular dynamics and mode-coupling theory

Heat Conduction in One-Dimensional Systems : molecular dynamics and mode-coupling theory. Jian-Sheng Wang National University of Singapore. Outline. Brief review of 1D heat conduction Introducing a chain model Nonequilibrium molecular dynamics results

590 views • 41 slides

I.L. Aleiner ( Columbia U, NYC, USA ) B.L. Altshuler ( Columbia U, NYC, USA )

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Mixed order phase transitions

Mixed order phase transitions. David Mukamel. Amir Bar, DM (PRL, 122, 01570 (2014)) . Phase transitions of mixed order . (a) diverging length as in second order transitions or (b) discontinuous order parameter as in first order transitions.

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Quantum impurity problems (QIP ) and numerical renormalization group (NRG): quick introduction

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The High Energy Limit of QCD

The High Energy Limit of QCD. The high energy limit is E -> infinity at fixed momentum transfer Not short distance limit which is E -> infinity at fixed angle. Related Questions :. How do gluons and quarks arise in hadrons?. What are the possible forms of high density matter?.

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Ginzburg-Landau theory of second-order phase transitions

Ginzburg-Landau theory of second-order phase transitions. Second order= no latent heat (ferromagnetism, superfluidity, superconductivity). Let the transition occur at T=T C. Ordered phase below transition (typically). Order parameter h (vanishes in disordered phase):.

1.77k views • 28 slides

Coarse-Grained Theory of Surface Nanostructure Formation

Coarse-Grained Theory of Surface Nanostructure Formation. Dimitri D. Vvedensky The Blackett Laboratory, Imperial College London Christoph A. Haselwandter Department of Applied Physics, Caltech. Imperial College London. Outline. Systems with many scales The coarse-graining road map

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Multiscale Modelling of Nanostructures on Surfaces

Multiscale Modelling of Nanostructures on Surfaces. Dimitri D. Vvedensky and Christoph A. Haselwandter Imperial College London. Outline. Multiscale Modelling: Quantum Dots Lattice Models of Epitaxial Growth Exact Langevin Equations on a Lattice Continuum Equations of Motion

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A nonequilibrium renormalization group approach to turbulent reheating

A nonequilibrium renormalization group approach to turbulent reheating. A case study in nonlinear nonequilibrium quantum field theory. Part I. J. Zanella, EC.

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The Origins of Lattice Gauge Theory

The Origins of Lattice Gauge Theory. Kenneth G. Wilson The Ohio State University. The Origins of Lattice Gauge Theory. 1974 - 2004 Homage 1973 - 1974 Origins 1958 - 1971 Thesis and After 2004 - Research Questions. I. 1974 - 2004 Homage. Current knowledge vs. 1974

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The Color Glass Condensate

The Color Glass Condensate. Outstanding questions:. What is the high energy limit of QCD?. How do gluons and quarks arise in hadrons?. What are the possible forms of high density matter?.

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The Color Glass Condensate and Glasma

The Color Glass Condensate and Glasma. CGC. Initial Singularity. Glasma. sQGP. Hadron Gas. 1. What is the high energy limit of QCD? What are the possible form of high energy density matter? How do quarks and gluons originate in strongly interacting particles?.

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Phase Transitions in Molecular Computing

Phase Transitions in Molecular Computing. Qualitative Difference in Properties of System as a Parameter is varied Tool for Analyzing Mixtures of Sticky-Ended Molecules Application for Sticky-Ended Molecular Computers. Approach for Analysis. Map Molecular Operations onto CA Model

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D.E. Vlasenko , V.I. Kuksa

Top pair production at ILC in the minimal gauge extension of the SM. D.E. Vlasenko , V.I. Kuksa Institute of Physics, Southern Federal University, Rostov-on-Don, Russia QFTHEP 2011. Problems of the SM. 1) 3 generations 2) special status of neutrino

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125 years of Excellence, Traditions, and Innovations

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