k Harvey, BNL Hot Quarks 2004 July Measurement of Invariant Differential Measurement of Invariant Differential Cross Sections of Identified Charged Cross Sections of Identified Charged Hadrons in p+p Collisions at RHIC Hadrons in p+p Collisions at RHIC Mark Harvey Mark Harvey Brookhaven National Brookhaven National Laboratory Laboratory July 18-24, 2004 July 18-24, 2004 Hot Quarks 2004 Workshop Hot Quarks 2004 Workshop Taos Valley, New Mexico, Taos Valley, New Mexico, USA USA
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Mark Harvey, BNL Hot Quarks 2004 July 18-24 Measurement of Invariant Differential Cross Sections of Identified Charged Hadrons in p+p Collisions at RHIC.
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Mark Harvey, BNL Hot Quarks 2004 July 18-24
Measurement of Invariant Differential Measurement of Invariant Differential Cross Sections of Identified Charged Cross Sections of Identified Charged Hadrons in p+p Collisions at RHICHadrons in p+p Collisions at RHIC
Mark HarveyMark Harvey
Brookhaven National Brookhaven National LaboratoryLaboratory
July 18-24, 2004 July 18-24, 2004
Hot Quarks 2004 WorkshopHot Quarks 2004 Workshop
Taos Valley, New Mexico, USATaos Valley, New Mexico, USA
Mark Harvey, BNL Hot Quarks 2004 July 18-24
Physics MotivationPhysics Motivation Differential Invariant Cross Section in p+p CollisionsDifferential Invariant Cross Section in p+p Collisions
– fundamental for understanding the particle production infundamental for understanding the particle production in p+p collisionsp+p collisions– baseline measurement for disentangling nuclear effects baseline measurement for disentangling nuclear effects
which arise in d+Au and Au+Au collisionswhich arise in d+Au and Au+Au collisions– Hard-scattered partons give rise to hadronic sprays; i.e., Hard-scattered partons give rise to hadronic sprays; i.e.,
jetsjets
Physics implications:Physics implications:– Careful examination of the Nuclear Modification factors; Careful examination of the Nuclear Modification factors;
e.g., Re.g., RdAudAu and R and RAuAuAuAu
– Initial state multiple scattering “broadens” the momentum Initial state multiple scattering “broadens” the momentum distribution and enhances the high pdistribution and enhances the high pT T yield compared to yield compared to point-like scaling from p+p collisionspoint-like scaling from p+p collisions
– Lack of high momentum enhancement Lack of high momentum enhancement jet suppression jet suppression
wherewhere LL = N = NeventsBBCeventsBBC//ppppBBCBBC
Application to A+A collisions:Application to A+A collisions:– The differential invariant yield in A+A collisions The differential invariant yield in A+A collisions
may be decomposed into a soft phenomenological may be decomposed into a soft phenomenological piece and a hard pQCD component piece and a hard pQCD component
Cross section sensitive to two important pieces of Cross section sensitive to two important pieces of physics!physics!– yields described in a two component model yields described in a two component model
Soft and hard production mechanismsSoft and hard production mechanisms
Mark Harvey, BNL Hot Quarks 2004 July 18-24
DDDD
UUUU
DDDDDDDDDDDD
DDDDUU
DDDDDDDDDDDD
DDDDUU
UUDDDD
UUUUUU
DDDD
UUUUUU
DDDD
UUUU
DDDDDDDDDDDD
DDDDUU
DDDDDDDDDDDD
DDDDUU
UUDDDD
UUUUUU
DDDD
UUUUUU
Participants
Spectators
Spectators
b
NuclearSystem A
NuclearSystem A
Hadronic Collisions
The number of spectator nucleons may be expressed as Nspect= 2A – Npart
Npart: No. of nucleons participating inelastically in interaction process DDDD
detector – TOF time resolution in Au+Au is 115 ps, relative to 2 cut in m2; K/ separation up to 2 GeV/c; p/K separation extends up to pT = 4 GeV/c… Beam-Beam Counter (BBC) provides start clock trigger
In p+p, clean pion and kaon separation out to |p| ~ 1.8 GeV/c; p/K In p+p, clean pion and kaon separation out to |p| ~ 1.8 GeV/c; p/K separation separation beyond 3 GeV/c -- TOF timing resolution ~135 psbeyond 3 GeV/c -- TOF timing resolution ~135 ps
m2 vs. momentum p+p @ √200 GeV
Mark Harvey, BNL Hot Quarks 2004 July 18-24
Differential Invariant Differential Invariant Cross Section in p+p Cross Section in p+p collisionscollisions
Pion spectra, exhibit concave shape well described by gamma-type function;
“ApT 2-λe-pT/T”
Proton spectra, Characterized by gamma function
Kaon spectra, Fall-off exponentially in pT
+, K+, p -, K-, p
At low pT (< 1.2 GeV/c), each particle species goes like f(pT) = e-bpT (b=6); similar to behavior observed at ISR energies
•particle production yield decreases with increasing centrality
•pions; power law for all centralities
•kaons and protons; pT
exponential in each centrality class
Mark Harvey, BNL Hot Quarks 2004 July 18-24
-/+; 0.97 0.001 0.02
K-/K+; 0.90 0.01 0.03
p/p; 0.72 0.01 0. 02
p+p Particle Ratiosp+p Particle Ratios
pion, Kaon and proton ratios are flat in pT
Shaded boxes represent systematic error estimates
PHENIX Preliminary
PHENIX Preliminary
PHENIX Preliminary
Mark Harvey, BNL Hot Quarks 2004 July 18-24
p p
/+ K-/K+ p/p
Particle Ratios for Particle Ratios for three Collision Systemsthree Collision Systems
slide prepared by Felix Matathias
Mark Harvey, BNL Hot Quarks 2004 July 18-24
d
Au
/+ K-/K+ p/p
Particle Ratios for Particle Ratios for three Collision Systemsthree Collision Systems
slide prepared by Felix Matathias
Mark Harvey, BNL Hot Quarks 2004 July 18-24
AuAu
/+ K-/K+ p/p
Particle Ratios for Particle Ratios for three Collision Systemsthree Collision Systems
slide prepared by Felix Matathias
Mark Harvey, BNL Hot Quarks 2004 July 18-24
AuAu
Like particle ratios: agree very well independent of collision system
Particle Ratios for Particle Ratios for three Collision Systemsthree Collision Systems
/+ K-/K+ p/p
slide prepared by Felix Matathias
Mark Harvey, BNL Hot Quarks 2004 July 18-24
•K/ Ratios increase steadily with increasing pT
•No apparent indication of saturation in this limited pT range
KK++//++ Ratios; 3 Collision systems Ratios; 3 Collision systems
•All three systems have comparable magnitudes – somewhat enhanced for most central Au+Au collisions slide prepared by Felix
Matathias
Mark Harvey, BNL Hot Quarks 2004 July 18-24
p/p/ Ratios for three Ratios for three Collision SystemsCollision Systems
•p+p, min bias d+Au and peripheral Au+Au are directly comparable •In p+p, p/ Ratios increase rapidly for pT < 1.4 GeV/c – flattens around 0.4 (0.3) for the positive (negative) particles at higher pT
Central Au+Au dramatically higher for pT > 1.4 GeV/c New Physics!
slide prepared by Felix Matathias
Mark Harvey, BNL Hot Quarks 2004 July 18-24
A look at RA look at RAAAA
●RAA considerably less than 1 for ’s; implication jet quenching due to hard scattered parton absorption in hot medium; p’s and K’s indicate other new physics.
• ’s are suppressed in central collisions; seem to be approaching unity for increasing pT in peripheral collisions
• K’s appear to flatten out within limited pT window in both central and peripheral collisions, respectively
• p’s increase fairly rapidly at low pT ; however, the protons are different and are consistent with no suppression!
Wor
k in P
rogre
ss
RRAAAA was computed in the was computed in the following way:following way:RRAAAA
SummarySummary Differential invariant cross section of identified Differential invariant cross section of identified
charged hadrons in p+p collisions charged hadrons in p+p collisions (paper (paper preparation for publication in process)preparation for publication in process)– baseline for d+Au and Au+Au baseline for d+Au and Au+Au – Excellent agreement between charged pion Excellent agreement between charged pion
average and published pi zero resultaverage and published pi zero result– High precision measurement of pions out to 10 High precision measurement of pions out to 10
orders of magnitude!orders of magnitude! Particle Ratios:Particle Ratios:
– Like particles; agree very well, independent of Like particles; agree very well, independent of collision systemcollision system
– K/K/ ratios rise steadily in limited p ratios rise steadily in limited pTT range range– p/p/ ratios saturate for all systems except Au+Au ratios saturate for all systems except Au+Au
central – may be viewed as flow effect since central – may be viewed as flow effect since protons are much heavier than pions; ergo, flow protons are much heavier than pions; ergo, flow contribution to their slope ~ m <ucontribution to their slope ~ m <utt>>2 2 ; see; see
Phys.Rev.C69:034909,2004
Mark Harvey, BNL Hot Quarks 2004 July 18-24
Summary ContinuedSummary Continued
Essentially, REssentially, RAAAA pions are suppressed in central pions are suppressed in central collisions – rising steadily peripheral… magnitude collisions – rising steadily peripheral… magnitude slightly increased for Kaons; however, they slightly increased for Kaons; however, they saturate in limited psaturate in limited pT T window; Protons are not window; Protons are not suppressed at higher psuppressed at higher pT T -- very different from -- very different from pions!pions!– Particle production mechanisms may be Particle production mechanisms may be
described with similar source in soft domain described with similar source in soft domain (p(pTT < 1.5 GeV/c) for < 1.5 GeV/c) for , K, K and p (pbar), and p (pbar), respectively – difference in production probably respectively – difference in production probably limited to large plimited to large pTT regime. regime.
More work to be done on RMore work to be done on RdAudAu and R and RAuAuAuAu before before physics result is ready for “prime time”physics result is ready for “prime time”