'Pair distribution' presentation slideshows

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Coulomb glass

Coulomb glass

Coulomb glass. Jacek Matulewski, Sergei Baranovski, Peter Thomas Departament of Physics Phillips-Universitat Marburg, Germany Faculty of Physics, Astronomy and Informatics Nicolaus Copernicus University in Toru?, Poland Marburg, V 2007. Computer simulations. Outline

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1.04k views • 81 slides
Characterization of Materials using the PDF

Characterization of Materials using the PDF

Characterization of Materials using the PDF. Thomas Proffen Manuel Lujan Jr. Neutron Scattering Center Los Alamos National Laboratory tproffen@lanl.gov. LA-UR 05-0111. Why do we care about the atomic structure?. Diamond hard transparent insulating expensive Graphite soft black

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808 views • 57 slides
Event-by-event flow from ATLAS

Event-by-event flow from ATLAS

Event-by-event flow from ATLAS. Jiangyong Jia. Initial geometry & momentum anisotropy. hydrodynamics. by MADAI.us. Single particle distribution. Pair distribution. Momentum anisotropy probes: initial geometry and transport properties of the QGP. Anisotropy power spectra.

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474 views • 37 slides
Theory of (strongly coupled) quark-gluon plasma (sQGP)

Theory of (strongly coupled) quark-gluon plasma (sQGP)

Theory of (strongly coupled) quark-gluon plasma (sQGP). From RHIC to LHC (31st J.Hopkins workshop, Heidelberg, Aug.2007) Edward Shuryak Stony Brook. The emerging theory of sQGP. Quantum mechanics. Stronly coupled cold trapped atoms. Manybody theory. Lattice simulations. sQGP.

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484 views • 35 slides
Computational Physics (Lecture 21)

Computational Physics (Lecture 21)

Computational Physics (Lecture 21) . PHY4370. where g ( r ) is the pair distribution and S ( k ) is the angular average of S ( k ). G ( r , t ) can be interpreted as the probability of observing one of the particles at r at time t if a particle was observed at r = 0 at t = 0 .

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433 views • 30 slides

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