BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 1 BRAHMS Particle Production Studied with BRAHMS I.G. Bearden, Niels.

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Presentation transcript:

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 1 BRAHMS Particle Production Studied with BRAHMS I.G. Bearden, Niels Bohr Institute For The BRAHMS collaboration

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 2 The BRAHMS Collaboration I.Arsene 10,I.G. Bearden 7, D. Beavis 1, C. Besliu 10, Y. Blyakhman 6, J.Brzychczyk 4, B. Budick 6,H. Bøggild 7,C. Chasman 1, C. H. Christensen 7, P. Christiansen 7, J.Cibor 4,R.Debbe 1,J. J. Gaardhøje 7,M. Germinario 7, K. Hagel 8, O. Hansen 7, H. Ito 11, E. Jacobsen 7, A. Jipa 10, J. I. Jordre 10, F. Jundt 2, C.E.Jørgensen 7, E. J. Kim 5, T. Kozik 3, T.M.Larsen 12, J. H. Lee 1, Y. K.Lee 5, G. Løvhøjden 2, Z. Majka 3, A. Makeev 8, B. McBreen 1, M. Murray 8, J. Natowitz 8, B. Neuman 11,B.S.Nielsen 7, K. Olchanski 1, D. Ouerdane 7, R.Planeta 4, F. Rami 2, D. Roehrich 9, B. H. Samset 12, S. J. Sanders 11, I. S. Sgura 10, R.A.Sheetz 1, Z.Sosin 3, P. Staszel 7, T.S. Tveter 12, F.Videbæk 1, R. Wada 8,A.Wieloch 3,Z. Yin 9 1 Brookhaven National Laboratory, USA, 2 IReS and Université Louis Pasteur, Strasbourg, France 3 Jagiellonian University, Cracow, Poland, 4 Institute of Nuclear Physics, Cracow, Poland 5 Johns Hopkins University, Baltimore, USA, 6 New York University, USA 7 Niels Bohr Institute, Blegdamsvej 17, University of Copenhagen, Denmark 8 Texas A&M University, College Station. USA, 9 University of Bergen, Norway 10 University of Bucharest, Romania, 11 University of Kansas, Lawrence,USA 12 University of Oslo Norway - 12 institutions-

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 3 Two small solid angle spectrometers (FS and MRS) 2.3° 30° that can rotate from 2.3° to 30° 90° 30° and 30° to 90° (MRS) provide excellent PID over broad range in y-p T The BRAHMS Experiment It’s Broad RAnge Hadron Magnetic Spectrometers!

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 4  K p BRAHMS Acceptance:

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 5 A BRAHMS Event TPM2 TPM1 D5 D1 T1 D2 T2 beam collision point (vertex) MRS at 90 degrees FFS at 6 degrees Reconstructed tracks

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 6 Event Counting We want to make spectra,  we need to count the number of collisions (events) N events and the number of tracks N tracks …still we need the centrality from the multiplicity (MA)… multiplicity [a.u.] …and the collision point (vertex) from the BB, ZDC and INEL counters. MA INEL ZDC BB We measure (almost) all the collisions and counting is easy!

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 7 Charged Particle Multiplicity dN/d  According to Bjorken,  >5GeV/fm 3 170MeV T BB

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 8 After appropriate corrections, we combine all data sets to obtain final invariant yields over a broad range of rapidity and p T Particle Spectra  K p

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 9 Pions: power lawKaons:exponentialProtons: Gaussian Top 5% central collisions Spectra:

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 10 Integrated multiplicities (Gaussian fit) N(   ) ~ 1780 N(  + ) ~1760 N(K + ) ~ 290 N(K  ) ~ 240 N(pbar) ~ 85 Rapidity Densities At y ~ 0, dN/dy is ~ 300 (300) for  + (  - ) ~ 47 (44) for K + (K  ) ~ 27 (20) for p (pbar) N(  ) >> N(K) > N(p) N(  + ) = N(   ) N(K + ) > N(K  ) and N(p) > N(pbar) systematically

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 11 BRAHMS, submitted to PRL, 31/12/03 nucl-ex/ P. Christiansen Ph.D. Thesis, København’s Universitet protons antiprotons Proton & antiproton dN/dy (5% central)

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 12 BRAHMS, submitted to PRL, 31/12/03 nucl-ex/ P. Christiansen Ph.D. Thesis, København’s Universitet “Net” Proton= proton - antiproton dN/dy (5% central) protons antiprotons net-proton

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 13 BRAHMS, submitted to PRL, nucl-ex/ P. Christiansen Ph.D. Thesis AGS : high stopping RHIC: more transparent RHIC vs. AGS,SPS:

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 14 Calculate net-baryon distribution from net-protons (and y=0 yields of , and Hijing…) Net Baryon dN/dy

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 15 Gaussians in p z : 2.03  0.16 Rapidity loss: gaussian in p z Rapidity loss :

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute  0.16 Rapidity loss: 6th order polynomial Rapidity loss : 6 order polynomial Gaussians in p z : 2.00  0.10 Total  E=25.7  2.1TeV

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 17  y vs. y beam Even (unphysically) extreme approximations don’t change conclusions: scaling broken, large energy available Total  E=25.7  2.1TeV

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 18 Fit , K and p distributions (dN/dy and  m T  vs y)  total energy of , K and p Assume reasonable distribution for particles we don’t detect (  0,n,  …) Calculate the total energy… NB: the method is very sensitive to the tails of the dN/dy dist. (  10-15%)  35 TeV (E beam  N part ) of which  25 TeV are carried by produced particles. p: 3108 p: 428 K + : 1628 K - : 1093  +: 5888  -: 6117  0 : 6004 n : 3729 n : 513 K 0 : 1628 K 0 : 1093  : 1879  : 342 Energy (in GeV) sum: 33.4 TeV produced: 24.8TeV Energy Balance…

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 19 Where is the energy? ≈ 9TeV in produced particles in the covered y range -3<y<3

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 20 Strange to non-strange meson ratios K - /  - ≈K + /  + at midrapidity Depend strongly on baryochemical potential

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 21 Y < 1 : consistent with Hadron Gas Stat. Model K + /  + : 15.6  0.1 % (stat) K/   : 14.7  0.1 % (stat) [Phys. Lett. B 518 (2001) 41] Divergence at higher y : Associated K + production No single source with unique T and  B Strangeness with Kaons RAPIDITY DEPENDENCE BRAHMS, PRL90 (2003) T~constant,  B varies with y Increasing y 63 GeV

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 22 Top 5% central collisions Kaon Spectra

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 23 Kaon Slopes Top 5% central collisions

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 24 Cover “peak” of strange matterhorn

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 25 Jets at RHIC p+p  jet+jet Au+Au  ??? nucleon parton jet Find this……….in this And, in BRAHMS, we only “see” this much…

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 26 h=0 h=2.2 Characterize “high” p T by single particle spectra

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 27 Nuclear Modification Quantified by: Cronin Enhancement Shadowing/Saturation Jet-quenching - yield relative to that from N+N collisions, scaled for the nuclear geometry (N bin ) Jet-quenching energy loss of high momentum particles in the dense medium due to - gluon brehmstralung in the colored medium - hadronic multiple scattering  suppression of leading hadrons - Au+Au at  s NN = 130GeV and 200GeV - next: energy+rapidity dependence

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 28 Arsene et al. PRL2003 To look at ‘only’ data, form ratio R  =R cp (  =2.2)/R cp (  =0)

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 29 d+Au Nuclear Modification  =0 High p T enhancement observed in d+Au collisions at  s NN =200 GeV. Comparing Au+Au to d+Au  strong effect of dense medium

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 30 submitted to PRL Cronin enhancement at  =0 - the “null” experiment that ruled out initial state effect as explanation for Au+Au suppression Increasing suppression for  3 - window to the low-x partons in the Au nuclei (Q S ~A 1/3 e -  y ) - consistent with CGC prediction R dAu at  s NN = 200 GeV

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 31 one week of 62.4 GeV running… New BRAHMS results No RHIC p+p running at this energy: - what should we use as reference?

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 32 Nuclear modification factor R AuAu - different centrality classes Energy dependence (SPS  RHIC) p T =3-4GeV/c 40-60%20-40%10-20%0-10% R AuAu at  s NN = 62.4 GeV

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 33 Conclusions  High energy density  70% of energy available for particle production  Source (nearly) same over >1 unit rapidity  63 GeV data: climb the K/  “matterhorn”?  High p T suppression persists to high y in Au+Au  More saturation as y increases in d+Au  Gluon saturation describes data, though not uniquely  Lots left to do…

BRAHMS 22. Oktober 2004 Forward Physics Workshop, KU I.G.Bearden, Niels Bohr Institute 34 In ’BT’ (Danish morning tabloid) Feb …….as plastic slippers with acrylic lining ? That you can recreate the Big Bang in a particle accelerator is simply a fantastic and earth shattering…. …discovery! At the same level.....