Forward and high pt physics at RHIC with BRAHMS

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November 8 200 4 Ericeira Jens Jørgen Gaardhøje, Niels Bohr Instit ute 1 Forward and high pt physics at RHIC with BRAHMS Stopping in Au+Au at √s=200, 62.4 GeV Rapidity dependence of high pt suppression of hadrons at √s=200 GeV Au+Au and d+Au at η=0 Au+Au at η=2.2, 3.2 d+Au at η= 0 to 3.2 (CGC?) Energy dependence of high pt suppression of hadrons at √s=62.4 GeV in Au+Au at η= 0, 1 Flavor dependence in Au+Au and d+Au Rapidity dependence of particle production in p+p collisions

description

Forward and high pt physics at RHIC with BRAHMS. Stopping in Au+Au at √s=200, 62.4 GeV Rapidity dependence of high pt suppression of hadrons at √s=200 GeV Au+Au and d+Au at η =0 Au+Au at η =2.2, 3.2 d+Au at η = 0 to 3.2 (CGC?) - PowerPoint PPT Presentation

Transcript of Forward and high pt physics at RHIC with BRAHMS

Page 1: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 1

Forward and high pt physics at RHIC with BRAHMS

Stopping in Au+Au at √s=200, 62.4 GeV

Rapidity dependence of high pt suppression of hadrons at √s=200 GeV

Au+Au and d+Au at η=0 Au+Au at η=2.2, 3.2 d+Au at η= 0 to 3.2 (CGC?)

Energy dependence of high pt suppression of hadrons at √s=62.4 GeV

in Au+Au at η= 0, 1

Flavor dependence in Au+Au and d+Au

Rapidity dependence of particle production in p+p collisions

Page 2: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 2

The BRAHMS experiment

Page 3: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 3

Excellent Hadron Identification by TOF and RICH

m2=p2( t2 / L2 -1)

D

p

KD

FS 4 deg

Page 4: Forward and high pt physics  at RHIC with BRAHMS

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 4

Transparency and beam energy loss at RHIC

BRAHMS PRL 93 (2004) 102301

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 5

Net Protons at 62.4 GeV

BRAHMS preliminary

0-5%

y

dN(p-pbar)/dy

Page 6: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 6

Rapidity and energy loss at RHIC

Rapidity loss saturates!

But Energy loss increases strongly

dE(baryon)=75GeV

ΔE(tot)=26TeV

Out of available

35 TeV

Relative rapidity loss :

35% < y/yb < 44%

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November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 7

Total relativistic energy

Produced particles

in -3<y<+3

carry about

9 TeV of total energy

E = mt cosh(y)

mt=(pt2+m2)1/2

Page 8: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 8

pt21

RAA

0

The smoking gun of QGP? Jet Quenching, high pt suppression.

ddp/d/N

ddp/NdR

TNN2NN

inelbin

T2

AA

Soft Hard (jets)

BRAHMS: PRL 91 (2003) 072305

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 9

Test: Absence of suppression at midrapidity in d+Au?

q

q

AuD

PRL 91 (2003) 072305

1/5

Absence of high pt suppression at midrapidity rules out initial

state effects .

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 10

What does theory have to say?

HIJING: pQCD (hard) + strings (soft),shadowing, very schematic jet quenching (1992)

Vitev-Gyulassy: pQCD (hard), no softCronin kT broadening, shadowing and (GLV) jet quenching

Cassing et al: pQCD (hard) + strings (soft)kT broadening, shadowing and energy loss (pre-hadronic and hadronic)

Hirano-Nara: pQCD (hard) + hydro (soft)Cronin kT broadening, shadowing and (GLV) jet quenching

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 11

High pt suppression persists at forward rapidity

Large high pt suppression also at forward rapidity.

Longitudinally extended medium, boost invariance, CGC or …?

Not quantitatively understood.

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November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 12

Energy loss by stimulated gluon emission in QGP ?

q

q

q

q

QCD: <E> g ln(1/L) dz

<L2>

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 13

RAuAu for hadrons at η=3.2 (4degrees)RHIC run IV

BRAHMS: preliminary

RCP indicates strong high pt suppression at very forward rapidities in

Au+Au

RCP= RdAu (0-20%) / (60-80%)

RdAu (30-50%) / (60-80%)

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 14

RAuAu @ 62.4 GeVη=0 and η=0.95

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 15

No sudden transition…..

√Snn (GeV)

?

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 16

Color Glass CondensateThe fundamental state of the colliding nuclei?

X= p(parton) /p(nucleon)

AuD

Measure at large y on D side:

Probes small x in Au

detector

Page 17: Forward and high pt physics  at RHIC with BRAHMS

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 17

Color Glass Condensate in d+Au collisions?

BRAHMS accepted PRL nucl-ex / 0403005

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November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 18

Centrality dependence … in d+Au

RCP= RdAu (0-20%) / (60-80%)

RdAu (30-50%) / (60-80%)

Most central to peripheral ratio is most enhanced at midrapidity and most suppressed at forward rapidity

This centrality inversion is consistent with the CGC model.

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 19

’High pt’ spectra are different for baryons and mesons in Au+Au

Very different from p+p and e++e-

Hadronic flow or partonic mechanism?

Qualitative agreement with parton recombination models, but need results from run IV for higher pt

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November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 20

How does it look in d+Au ? Identified hadrons at 4 degrees (η=3.2)

π

K

p

PID with RICH

At eta= 3.2

P-bar : 10%

Π- : 80%

Page 21: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 21

RdAu at η=3.2(min.bias) Baryon meson difference in d+Au

Strong Difference between

mesons (pions) and Baryons

(anti-p) persists at forward rapidity

in d+Au collisions

BRAHMS preliminary

Flow?

Isospin?

Need to understand

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 22

The hadron spectrum for d+Au at η=3.2

But many protons at forward rapidity

Excess of h+ over h-

Page 23: Forward and high pt physics  at RHIC with BRAHMS

November 8 2004

Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 23

Difference understandable from relative abundances

h+ = 0.8h-( 1 + p/+ + K/+)

Page 24: Forward and high pt physics  at RHIC with BRAHMS

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 24

p+p at 200GeVParticle ratios vs rapidity

PYTHIA misses 200GeV protons

BRAHMS, nucl-ex/0409002, Submitted to Phys. Lett. B (2004)

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 25

Proton/pion in p+p at η=3.2vs. Pythia (vs. 6.303)

Page 26: Forward and high pt physics  at RHIC with BRAHMS

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 26

Summary

Large high pt suppression at midrapidity in Au+Au. Gluon radiation energy loss?

No suppression in d+Au => no initial state effects. Large effect (factor 5).

Strong high pt suppression in Au+Au persists at forward rapidities- need quantitative understanding.

Reduced high pt suppression in Au+Au at 62.4 GeV

Decrease in R(dAU) from η=0 to η=3.2 and centrality dependence inversion. Consistency with CGC picture.

Baryon/mesons difference sseen at midrapidty in Au+Au is also present in d+Au at forward rapidity.

Pythia does not reproduce protons in p+p.

=== > BRAHMS whitepaper on RHIC discoveries: Nucl-ex/0410020, subm. Nucl. Phys. A

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 27

Extra material

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 28

Is a unified picture emerging?

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 29

New Physics?

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 30

I.G. Bearden7, D. Beavis1, C. Besliu10, Y. Blyakhman6, J. Bondorf7, J.Brzychczyk4, B. Budick6, H. Bøggild7, C. Chasman1, C. H. Christensen7, P. Christiansen7, J.Cibor4, R.Debbe1, J. J. Gaardhøje7, M. Germinario7, K. Grotowski4, K. Hagel8, O.

Hansen7, A. Holm7, A.K. Holme12, H. Ito1, E. Jacobsen7, A. Jipa10, J. I. Jordre9, F. Jundt2, E. Johnson11, C. E. Jørgensen7,T. Keutgen9, E. J. Kim11, T. Kozik3, T.M.Larsen12, J. H. Lee1, Y. K.Lee5, G. Løvhøjden12, Z. Majka3, A. Makeev8, B. McBreen1, M. Murray11, J. Natowitz8, B.S.Nielsen7, K. Olchanski1, D. Ouerdane7, R.Planeta4, F. Rami2, D. Roehrich9, B. H.

Samset12, S. J. Sanders11, D. Sandberg7,I. S. Sgura10, R.A.Sheetz1, Z.Sosin3, P. Staszel7,3, T.S. Tveter12, F.Videbæk1, R. Wada8 and A.Wieloch3.

1Brookhaven National Laboratory, USA 2IReS and Université Louis Pasteur, Strasbourg, France

3Jagiellonian University, Cracow, Poland 4Institute of Nuclear Physics, Cracow, Poland 5Johns Hopkins University, Baltimore, USA

6New York University, USA 7Niels Bohr Institute, Blegdamsvej 17, University of Copenhagen, Denmark 8Texas A&M University, College Station. USA

9University of Bergen, Norway 10University of Bucharest, Romania

11University of Kansas, Lawrence,USA 12 University of Oslo Norway

BRAHMS Intl. collaboration

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 31

At lower energy the opposite is seen :High pt enhancement

CERN- SPS

(snn=17 GeV)

High p_t enhancement seen when compared to p+p scaled by N_binary.

Cronin effect:

quark mult scattering

Page 32: Forward and high pt physics  at RHIC with BRAHMS

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 32

p+p reference at 62.4 GeV: a problem

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 33

Transverse spin asymmetry for pions using polarized p+p collisions

STAR PRL 92,06230(2004)D.L.Adams (E704) Phys.Lett B264,462(1991);

Phys.ReV D53, 4747 (1996). FNAL704

AANN = (s+ - s-) / (s+ + s-) = (s+ - s-) / (s+ + s-)

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 34

First results at high XF

<ε >~ -0.035 AN = -0.08 +- 0.005 +- [0.015]

0.17 < xF < 0.32

< ε >~ +0.022 AN = +0.05 +- 0.005 +- [0.015]

0.17 < xF < 0.32

BRAHMS preliminary

AANN = = εε /P P=0.40 - 0.45 /P P=0.40 - 0.45

εε = (N+ /L+ - N-/L-) / (N+ /L+ + N-/L-) = (N+ /L+ - N-/L-) / (N+ /L+ + N-/L-)

= (N+ - L*N-) / (N+ + L*N-) with L = L+ / L-= (N+ - L*N-) / (N+ + L*N-) with L = L+ / L-

π+

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Ericeira Jens Jørgen Gaardhøje, Niels Bohr Institute 35

BRAHMS whitepaperon RHIC discoveries

Conclusion: …There is no doubt that the experiments at RHIC have revealeda plethora of new phenomena that for the most part have come as asurprise. In this sense it is clear that the matter that iscreated at RHIC differs from anything that has been seen before.What name to give it must await our deeper understanding of thismatter.

Nucl-ex/0410020, subm. Nucl. Phys. A