1 FORWARD-BACKWARD RAPIDITY CORRELATIONS IN A TWO STEP SCENARIO Jorge Dias de Deus José Guilherme Milhano CERN, 2007.

Slides:



Advertisements
Similar presentations
1/10Boris Tomášik: Identifying fireball fragmentation with the Kolmogorov-Smirnov test Boris Tomášik Univerzita Mateja Bela, Banská Bystrica, Slovakia.
Advertisements

Test practice Multiplication. Multiplication 9x2.
Elliptic flow of thermal photons in Au+Au collisions at 200GeV QNP2009 Beijing, Sep , 2009 F.M. Liu Central China Normal University, China T. Hirano.
1/03/09 De 89 à 98. 1/03/09 De 89 à 98 1/03/09 De 89 à 98.
Lecture 3 Jack Tanabe Old Dominion University Hampton, VA January 2011 Conformal Mapping.
Forward-Backward Correlations in Relativistic Heavy Ion Collisions Aaron Swindell, Morehouse College REU 2006: Cyclotron Institute, Texas A&M University.
Multiplicity Distributions and Percolation of Strings J. Dias de Deus and C. Pajares CENTRA,Instituto Superior Tecnico,Lisboa IGFAE,Universidade de Santiago.
Terence Tarnowsky Long-Range Multiplicity Correlations in Au+Au at Terence J Tarnowsky Purdue University for the STAR Collaboration 22nd Winter Workshop.
Resolution of Several Puzzles at Intermediate p T and Recent Developments in Correlation Rudolph C. Hwa University of Oregon Quark Matter 05 Budapest,
Current status of the long- range correlations analysis in Be+Be at 150 AGeV/c E. Andronov, A. Seryakov NA61/NA49 Collaboration meeting Dubna, 10/04/14.
CHAPTER 3 STATES OF MATTER SOLIDS- definite shape and volume LIQUIDS- definite volume but no definite shape. Takes the shape of the container GASSES- takes.
Correlation Coefficient Negative No Positive Correlation Correlation Correlation.
Physics 361 Principles of Modern Physics Lecture 8.
Forward - Backward Multiplicity in High Energy Collisions Speaker: Lai Weichang National University of Singapore.
Rapidity correlations in the CGC N. Armesto ECT* Workshop on High Energy QCD: from RHIC to LHC Trento, January 9th 2007 Néstor Armesto Departamento de.
Narrowing of Balance Function and Hadronization Time at RHIC Energy Du Jiaxin, and Liu Lianshou Institute Of Particle Physics, Huazhong Normal University.
Definitions of the Day (DODs) 8.7 – More Multiplication Properties of Exponents Power to a Power Product to a Power.
ZIMANYI-SCHOOL11, Budapest, 01/12/2011 A. Ster, RMKI, Hungary 1 Correlations in double parton distributions at small x MTA KFKI RMKI, Budapest, Hungary.
As one evolves the gluon density, the density of gluons becomes large: Gluons are described by a stochastic ensemble of classical fields, and JKMMW argue.
Flow fluctuation and event plane correlation from E-by-E Hydrodynamics and Transport Model LongGang Pang 1, Victor Roy 1,, Guang-You Qin 1, & Xin-Nian.
Longitudinal de-correlation of anisotropic flow in Pb+Pb collisions Victor Roy ITP Goethe University Frankfurt In collaboration with L-G Pang, G-Y Qin,
Glasma Definition: The matter which is intermediate between the Color Glass Condensate and the Quark Gluon Plasma It is not a glass, evolving on a natural.
Formula? Unit?.  Formula ?  Unit?  Formula?  Unit?
STRING PERCOLATION AND THE GLASMA C.Pajares Dept Particle Physics and IGFAE University Santiago de Compostela CERN The first heavy ion collisions at the.
Workshop for Particle Correlations and Femtoscopy 2011
LONG RANGE CORRELATIONS;EVENT SIMULATION AND PARTON PERCOLATION C.Pajares Dept Particle Physics and IGFAE University Santiago de Compostela,Spain BNL Glasma.
Long Range Correlations,Parton Percolation and Color Glass Condensate C.Pajares Dept Particle Physics and IGFAE University Santiago de Compostela,Spain.
STRING COLOR FIELDS PREDICTIONS for pp at LHC C.Pajares University Santiago de Compostela Quantum Field Theory in Extreme Environments,Paris April 2009.
The CGC and Glasma: Summary Comments The CGC, Shadowing and Scattering from the CGC Inclusive single particle production J/Psi Two Particle Correlations.
String Theory Mihir John What are the most basic constituents that make up the universe around us?
Flow fluctuation and event plane correlation from E-by-E Hydrodynamics and Transport Model Victor Roy Central China Normal University, Wuhan, China Collaborators.
Methods of Studying Net Charge Fluctuations in Nucleus-Nucleus Collisions Event-by-event fluctuations of the net charge in local regions of phase space.
Methods of Studying Net Charge Fluctuations in Nucleus-Nucleus Collisions Event-by-event fluctuations of the net charge in local regions of phase space.
FIN 614: Financial Management Larry Schrenk, Instructor.
Higher and National 5 Course Assessment: Question Paper.
Chemistry: Chapter 3 States of Matter.
Chemistry I Honors Kinetics. What is Kinetics? This is a totally different study than anything we have done. Some of it uses concepts from Unit 1, but.
System-size dependence of strangeness production, canonical strangeness suppression, and percolation Claudia Höhne, GSI Darmstadt.
The Color Glass Condensate and Glasma What is the high energy limit of QCD? What are the possible form of high energy density matter? How do quarks and.
8-1 Direct, Inverse, and Joint Variation Some relationships in mathematics can be described as examples of direct variation. This means that y is a multiple.
First analysis of Long-Range (Forward-Backward) pt and multiplicity correlations in ALICE in pp collisions at 900 GeV G.Feofilov, A.Ivanov, V.Vechernin.
QM2008 Jaipur, India Feb.4– Feb. 10, STAR's Measurement of Long-range Forward- backward Multiplicity Correlations as the Signature of “Dense Partonic.
Implications for LHC pA Run from RHIC Results CGC Glasma Initial Singularity Thermalized sQGP Hadron Gas sQGP Asymptotic.
Objectives  By the end of this class you should be able to:  State the law of reflection.  State the principle of superposition.  Know whether two.
L. Apolinário, N. Armesto, J. G. Milhano, C. Salgado TOWARDS JET CALCULUS IN A QCD MEDIUM.
9.1 Inverse Variation. Inverse variation When one value increases, the other decreases.
Azimuthal correlations of forward di-hadrons in d+Au collisions at RHIC Cyrille Marquet Theory Division - CERN Based on :C.M., Nucl. Phys. A796 (2007)
Viscous Hydrodynamic Evolution for the CGC at RHIC and LHC Akihiko Monnai Department of Physics, The University of Tokyo Collaborator: Tetsufumi Hirano.
LESSON 5 - STATISTICS & RESEARCH STATISTICS – USE OF MATH TO ORGANIZE, SUMMARIZE, AND INTERPRET DATA.
。 33 投资环境 3 开阔视野 提升竞争力 。 3 嘉峪关市概况 。 3 。 3 嘉峪关是一座新兴的工业旅游城市,因关得名,因企设市,是长城文化与丝路文化交 汇点,是全国唯一一座以长城关隘命名的城市。嘉峪关关城位于祁连山、黑山之间。 1965 年建市,下辖雄关区、镜铁区、长城区, 全市总面积 2935.
1 Brijesh K Srivastava Department of Physics & Astronomy Purdue University, USA in collaboration with A. S. Hirsch & R. P. Scharenberg ( Purdue University)
How to extract physics from ν d y n Peter Christiansen, Lund Work done together with Eva Haslum and Evert Stenlund.
Nuclear Effects in Hadron Production at HERMES
. - t !!l t. - 1f1f J - /\/\ - ' I __.
Experimental Studies of Quark Gluon Plasma at RHIC
DSMC Collision Frequency Traditional & Sophisticated
.. '.. ' 'i.., \. J'.....,....., ,., ,,.. '"'". ' · · f.. -··-·· '.,.. \...,., '.··.. ! f.f.
Strong color fields in AA and pp high multiplicity events
New d+Au RHIC data show evidence for parton saturation
Queuing Analysis.
Lecture 3 Jack Tanabe Old Dominion University Hampton, VA January 2011
Ашық сабақ 7 сынып Файлдар мен қапшықтар Сабақтың тақырыбы:
Windows басқару элементтері
Delayed Load What will happen if lw $6 $0($1) add $4 $6 $1
5.5-Multiple Angle Formulas
Bernoulli Trials Two Possible Outcomes Trials are independent.
On the Measure of Dynamical Event-by-Event pt Fluctuations
Қош келдіңіздер!.
Информатика пән мұғалімі : Аитова Карима.
6.2.1 Reaction Theories.
Presentation transcript:

1 FORWARD-BACKWARD RAPIDITY CORRELATIONS IN A TWO STEP SCENARIO Jorge Dias de Deus José Guilherme Milhano CERN, 2007

2 TWO STEP SCENARIO?... AS A RESULT OF COLLISIONS 1) FORMATION OF EXTENDED OBJECTS IN RAPIDITY, FIRST; 2) FOLLOWED BY LOCAL EMISSION OF PARTICLES [This happens in GLASMA model, SCHWINGER strings, …] FORWARD-BACKWARD RAPIDITY CORRELATIONS: [Two rapidity windows with a rapidity gap between] F = a + bn F b ≡ D 2 FB / D 2 FF

3 BASIC FORMULAE NUMBER OF COLLISIONS ~ NUMBER OF STRINGS: : reduction factor, determined by multiplicity

4 where and we have assumed Poisson distribution for local emission. MAIN RESULT: [CGC model: ]

5 APLLICATION: y B FIXED, MID RAPIDITY y F VARYING, MOVING INTO HIGHER RAPIDITY REWRITE x ≡ / varying, 1 < x < ∞ K’ = k / fixed Ex: k’ = 1

6