'2 fm' presentation slideshows

Lecture 2 on J/  suppression

Michel GONIN. Lecture 2 on J/  suppression. 1. Charmonium bound states. 2. Screening effects in the plasma. 3. Experimental results. 4. Life (for physicist) is tough. l D depends on the temperature. . quarkonia. q. q. Lattice QCD.  ’. . T > T c. .  = 0.

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Chapter 3. Continuous-wave modulation

carrier frequency. message signal. Chapter 3. Continuous-wave modulation. 3.1 Introduction modulation: the process by which some characteristic of a carrier is varied in accordance with a modulating wave(signal) 3.2 Amplitude Modulation 1. Am 1) Sinusoidal carrier wave

1.36k views • 57 slides

Summary- DIS05

Summary- DIS05. Allen Caldwell Max-Planck-Institute f. Physik. Goal of this talk. My list of the key physics topics addressed by DIS physics Where we stand - selected results Ideas for the future. The Key Topics - my opinion.

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Femtoscopy in HIC. Theory R. Lednický, JINR Dubna & IP ASCR Prague

Femtoscopy in HIC. Theory R. Lednický, JINR Dubna & IP ASCR Prague. History QS correlations FSI correlations Correlation asymmetries Summary. History. Correlation femtoscopy :. measurement of space-time characteristics R, c ~ fm. of particle production using particle correlations.

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What we learned from HERA-1 ? What is coming from HERA-2 ? What is left out ?

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Bulk and Spectral Observables in Lattice QCD

WMAP (2001-). RHIC (2000- ). LATTICE. Bulk and Spectral Observables in Lattice QCD. Tetsuo Hatsuda ( ???? ) Univ. Tokyo ? ??????. Three Major Tools to study Early Universe. Contents. [1] Introduction -- lattice approach to hot QCD [2] Bulk properties of hot QCD

544 views • 40 slides

Correlation Femtoscopy R. Lednický, JINR Dubna & IP ASCR Prague

Correlation Femtoscopy R. Lednický, JINR Dubna & IP ASCR Prague. History QS correlations FSI correlations Correlation asymmetries Summary. History. Correlation femtoscopy :. measurement of space-time characteristics R, c ~ fm. of particle production using particle correlations.

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From HERA to eRHIC A. Caldwell, Max-Planck-Institut f. Physik

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Azimuthally-sensitive HBT (asHBT) in Au+Au collisions at ?s NN =200 GeV

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Unpolarized Physics Program HERA-3 Workshop, MPI, 17-Dec-2002 A. Caldwell

Unpolarized Physics Program HERA-3 Workshop, MPI, 17-Dec-2002 A. Caldwell. Physics Topics: eP, eD, eA Detector Requirements Accelerator Requirements Sources: Future Physics at HERA Workshop (95/96) EIC White Paper THERA contribution to TESLA TDR

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Comparing energy loss phenomenology

Comparing energy loss phenomenology. Marco van Leeuwen Utrecht University. Energy loss in QCD matter. radiated gluon. propagating parton. m 2. QCD bremsstrahlung (+ LPM coherence effects). Transport coefficient. l. Energy loss. Energy loss probes:. Density of scattering centers:.

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Tilted Pion Sources and Azimuthal Dependence of HBT Radii

Tilted Pion Sources and Azimuthal Dependence of HBT Radii. Mike Lisa. Formalism: R 2 ( f ) ? spatial correlation tensor implicit & explicit f -dependence a dominant and overlooked correlation ? striking experimental signal toy models, RQMD pion flow and spatially tilted sources

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Some critical phenomena in AA and pp collisions and percolation string model

Some critical phenomena in AA and pp collisions and percolation string model. G.A. Feofilov, O.A. Kochebina Reporter O.A. Kochebina. St. Petersburg State University. The 5th International Nordic "LHC and Beyond" Workshop "The First LHC Physics and Major Spin-Offs", 9 June 2010. Outline.

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Characterizing the freezeout at RHIC: HBT, spectra, and elliptic flow

Characterizing the freezeout at RHIC: HBT, spectra, and elliptic flow. Mike Lisa, Ohio State University STAR Collaboration. U.S. Labs: Argonne, Lawrence Berkeley National Lab, Brookhaven National Lab U.S. Universities: Arkansas, UC Berkeley, UC Davis, UCLA, Carnegie Mellon,

428 views • 24 slides

F 2 /F L with HERA III/eRHIC A. Caldwell, Max-Planck-Institut f. Physik

F 2 /F L with HERA III/eRHIC A. Caldwell, Max-Planck-Institut f. Physik. New Detector for HERA/eRHIC. Physics - QCD in the high energy limit. Kinematics. E e =10 - 27.5 GeV E P =250 - 920 GeV. r. *. s=(k+P) 2 = (100-320 GeV) 2 CM energy squared Q 2 =-(k-k`) 2 virtualiy

361 views • 23 slides

Two Particle Interferometry at RHIC

Two Particle Interferometry at RHIC. Sergey Panitkin (Brookhaven National Laboratory). Outline. Introduction and Motivation Summary of Results from AuAu 130 GeV Results from AuAu 200 GeV PHOBOS PHENIX STAR (see talks by M. Lisa, V. Okorokov) Summary and outlook. q Side. q Out. p y.

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Heavy Quark Evolution and Flow in Hot and Dense Medium

Heavy Quark Evolution and Flow in Hot and Dense Medium. Shanshan Cao In Collaboration with Guangyou Qin and Steffen A. Bass Duke University. Outline. Introduction and motivation Methodology Improved Langevin approach incorporating gluon radiation mechanism

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HBT in pp collisions?

?+/p. NA22. e+/e-. AMY. E735. UA1. OPAL. HBT in pp collisions?. Just a sampling. Dowell., Proc. Of the VII Topical Workshop on Proton-AntiProton Collider Physics, p115, Word Scientific 1989.

212 views • 10 slides