Title: PHOBOS WHITE PAPER REPORT
1PHOBOS WHITE PAPER REPORT
White paper report, June 2004
- Wit Busza
- on behalf of the PHOBOS Collaboration
2- We have discovered a strongly interacting medium
with extremely high energy density whose
description in terms of simple hadronic degrees
of freedom is not appropriate - Furthermore, we have discovered that much of the
data can be expressed in terms of simple scaling
rules which suggest the existence of strong
global constraints or some kind of universality
in the mechanism of the production of hadrons in
high energy collisions (possible connection to
ideas of parton saturation)
- To date, in Heavy Ion Collisions, there is no
evidence for the weakly interacting QGP, as
naively imagined by a large segment of the
community before RHIC turn-on and concluded from
a possible misinterpretation of the lattice
results (80 of Stefan-Boltzmann is not weakly
interacting)
3Key earlyPHOBOS observation
4Particle Density near Mid-Rapidity
PRL 85, 3100 (2000)
PRL 88, 22302 (2002)
PRL 91, 052303 (2003)
arXivnucl-ex/0405027
5Energy per unit volume
dNch/dh
Number of Particles Produced at y0
ltEgt 0.7 GeV
Therefore total energy released in h lt 1 is
2000GeV
Energy of Collision
relevant initial volume pR2 X (0.1fm - few
fm) X 2
Initially released energy per unit volume gt few
GeV/fm3 Note energy density inside proton 0.5
GeV/fm3
Data from PRL 85, 3100 (2000) PRL 88, 22302
(2002) PRL 91, 052303 (2003)
arXivnucl-ex/0405027
6- In AuAu Collisions at ?sNN 200 GeV
- Maximum released energy is at mid-rapidity
- In a system at rest with the center of mass
- Energy/volume gt few GeV/fm3
- It is not appropriate to describe such a
system in terms of simple hadronic degrees of
freedom
7AT MID-RAPIDITY THE SYSTEM IS RELATIVELY
BARYON-FREE
PRC 67, 021901R (2003)
8The high energy system is strongly interacting
9Evidence from flow
200 GeV AuAu PHOBOS preliminary
0 lt h lt 1.5
0-55 central, h h-
PRL 89, 222301 (2002) Nucl. Phys. A715, 611c
(2003)
10Evidence from the small number of particles
produced with very low pT
In a large volume, weakly interacting system you
would expect the development of particles with
long wavelength
PHOBOS PHENIX
arXivnucl-ex/0401006
11Evidence from the suppression of high-pT
particles
PHOBOS dAu 200 GeV
AuAu 0-6 200 GeV
PRL 91, 072302 (2003)
12BACK-TO-BACK JET CORRELATIONS
STAR
PRL 90, 082302 (2003)
13Discovery of simple scaling rulesin other
words, discovery of global constraints
14DISCOVERY OF SIMPLE SCALING BEHAVIORS
- UNIVERSAL TOTAL PARTICLE PRODUCTION
- ABSENCE OF BOOST INVARIANT CENTRAL PLATEAU
- UNIVERSAL SCALING ACCORDING TO LIMITING
FRAGMENTATION - UNIVERSAL Npart SCALING
- FACTORIZATION INTO GEOMETRIC PART AND ENERGY PART
15UNIVERSAL TOTAL PARTICLE PRODUCTION
16Relevant energy for comparisons of AuAu, pp,
and dAu
In pp collisions, on average, approximately half
the energy goes into the leading baryon
A.Brenner et a., Phys.Rev.D26 (1982) 1497l
arXivnucl-ex/0301017 arXivnucl-ex/0403033
17arXivnucl-ex/0301017
18ABSENCE OF BOOST INVARIANT CENTRAL PLATEAU
19PHOBOS
Plateau in pseudorapidity distributions is
misleading Rapidity distributions of pions are
gaussians
PRL 91, 052303 (2003) arXivnucl-ex/0403050
20No boost-invariant central plateau for v2
PHOBOS Preliminary v2200
PHOBOS v2130
PRL 89, 222301 (2002)
21UNIVERSAL SCALING ACCORDING TO LIMITING
FRAGMENTATION
22PRL 91, 052303 (2003)
23Rest frame of A
Rest frame of p or d
arXivnucl-ex/0403033
24(No Transcript)
25Energy and pseudorapidity dependence of v2
To be submitted PRL June 2004
26Limiting fragmentation seen in v2
To be submitted PRL June 2004
27Elliptic flow
PRL 91, 052303 (2003)
To see the limiting behavior, imagine that RHIC
collided beams with asymmetric energy, with h
-2 corresponding to y 0.
28Universal Npart scaling
29Npart scaling for pA, KA, pA, dA, AA 10 GeV to
200 GeV Npart from 2 to 350
Preliminary
Phobos and E178 data
pp chosen to have the same available energy
E178 J.E.Elias et al., Phys.Rev.D22(1980) 13
arXivnucl-ex/0403033
30FACTORIZATION INTO GEOMETRIC PART AND ENERGY PART
31arXivnucl-ex/0403033
32Example of factorization into geometric part and
energy part
SAME SEEN IN pA AT ALL ENERGIES
arXivnucl-ex/0403033
33Phobos
PRL 91, 052303 (2003)
Nucl.Phys. A715 (2003) 65-74
34Centrality Dependence at h lt 1
Ratio of 200/130 and 200/19.6
PRC 65, 061901R (2002) arXivnucl-ex/0405027
35Energy and geometry factorize
arXivnucl-ex/0405003
36- We have discovered a strongly interacting medium
with extremely high energy density whose
description in terms of simple hadronic degrees
of freedom is not appropriate - Furthermore, we have discovered that much of the
data can be expressed in terms of simple scaling
rules which suggest the existence of strong
global constraints or some kind of universality
in the mechanism of the production of hadrons in
high energy collisions
- To date, in Heavy Ion Collisions, there is no
evidence for the weakly interacting QGP, as
naively imagined by a large segment of the
community before RHIC turn-on and concluded from
a possible misinterpretation of the lattice
results (80 of Stefan-Boltzmann is not weakly
interacting)
37WE DO NOT CLAIM THE FOLLOWING
- Phenomena unique to RHIC
- - could be similar to the
story of jets - Color deconfinement
- - exact nature of system
unknown - Chiral symmetry restoration
38SPARES
39Collaboration (May 2004)
Birger Back, Mark Baker, Maarten Ballintijn,
Donald Barton, Russell Betts, Abigail Bickley,
Richard Bindel, Wit Busza (Spokesperson), Alan
Carroll, Zhengwei Chai, Patrick Decowski,
Edmundo García, Tomasz Gburek, Nigel George,
Kristjan Gulbrandsen, Clive Halliwell, Joshua
Hamblen, Adam Harrington, Michael Hauer, Conor
Henderson, David Hofman, Richard Hollis, Roman
Holynski, Burt Holzman, Aneta Iordanova, Jay
Kane, Nazim Khan, Piotr Kulinich, Chia Ming Kuo,
Willis Lin, Steven Manly, Alice Mignerey, Gerrit
van Nieuwenhuizen, Rachid Nouicer, Andrzej
Olszewski, Robert Pak, Inkyu Park, Heinz
Pernegger, Corey Reed, Christof Roland, Gunther
Roland, Joe Sagerer, Helen Seals, Iouri Sedykh,
Wojtek Skulski, Chadd Smith, Maciej Stankiewicz,
Peter Steinberg, George Stephans, Andrei
Sukhanov, Marguerite Belt Tonjes, Adam Trzupek,
Carla Vale, Sergei Vaurynovich, Robin Verdier,
Gábor Veres, Peter Walters, Edward Wenger, Frank
Wolfs, Barbara Wosiek, Krzysztof Wozniak, Alan
Wuosmaa, Bolek Wyslouch ARGONNE NATIONAL
LABORATORY BROOKHAVEN NATIONAL LABORATORY INSTITU
TE OF NUCLEAR PHYSICS PAN, KRAKOW MASSACHUSETTS
INSTITUTE OF TECHNOLOGY NATIONAL CENTRAL
UNIVERSITY, TAIWAN UNIVERSITY OF ILLINOIS AT
CHICAGO UNIVERSITY OF MARYLAND UNIVERSITY OF
ROCHESTER
40dN/dh
UA5
41- In a wide variety of systems (hadron A to AA)
the total number of emitted charged particles
appears to scale linearly with the number of
participants. - The total multiplicity of charged particles
emitted in hadron A is equal to the number of
participants times the multiplicity observed in
pp, while in AA, the constant of
proportionality is the multiplicity produced in
ee- annihilations or in pp at twice the center
of mass energy. This is suggestive of a universal
energy dependence of charged particle
multiplicities in strong interactions. - In the forward region, the pseudorapidity
densities, when measured as a function of the
shifted variable etaeta-ybeam appear not to
depend on beam energy. The precise form of the
distribution depends on the impact parameter, but
again in an energy- independent way. No evidence
is seen for a boost invariant central plateau.