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Strangeness Production in Heavy-Ion Collisions at STAR. Introduction.. Bulk strangeness production… Mid- p T spectra… Hard processes and strangeness… Summary…. Anthony Timmins for the STAR Collaboration. Introduction. STAR Preliminary. - PowerPoint PPT Presentation
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STAR
Strangeness Production in Heavy-Ion Collisions at STAR
Anthony Timmins for the STAR Collaboration
Introduction.. Bulk strangeness production… Mid-pT spectra…
Hard processes and strangeness… Summary…
STAR
2/13
Introduction Strangeness production helps us
explore many processes…
– low q2
Strangeness enhancement Flow Recombination
– high q2
Jet quenching Flavor changing
New STAR data in this talk
– Cu+Cu 62 GeV
– High-pT p+p 200 GeV
– High-pT Au+Au 200 GeV
STAR Preliminary
STAR
3/13
Strangeness enhancement key measurement at 200 GeV
Old idea (Phys. Rev. Lett. 48 (1982) 1066)
– s+s production cross section increases in QGP
– s+s in QGP reaches thermal expectations on small time scale…
s ~3 fm/c (QGP) s ~20-200 fm/c (hadron gas)
Can it be understood via phase space restrictions?
– Canonical Formalism Strangeness in p+p suppressed
relative to A+A? (Phys. Lett. B486 (2000) 61)
Bulk strangeness productionAs a QGP signature…
STAR
4/13
Bulk strangeness production Enhancement at 200 GeV… New d+Au 200 GeV data (not shown)
– See Xianglei Zhu’s talk later in session
Cu+Cu and Au+Au and enhancements (E) approximately described by simple function:
Predicts…
– Rise in E with <Npart>
– Higher E for central Cu+Cu
– Above 1 E for d+Au 200 GeV
Fraction of participants that undergo multiple collisions
STAR Preliminary
K0S B = 2.10
B = 2.45
B = 5.05
B = 13.1
Multiple Collisions
Single Collisions
f=1/4
STAR
5/13
Bulk strangeness production dN/dy at 62 GeV…
STAR Preliminary
No p+p 62 GeV reference data yet
– Can still investigate dN/dy per <Npart>
and K0Sper participant
yields can be described by
– C f(Npart) + D
Reproduces qualitative features of yields per <Npart>
Turning to multi-strange…
Cu+Cu K0S and : Stat errors only
Au+Au K0S and : Stat+Sys errors
New Cu+Cu 62 GeV data
Cu+Cu and : Stat errors only
Au+Au and : Stat errors only
STAR
6/13
Bulk strangeness productionWhat about the ?
Enhanced in heavy-ion collisions at 62 and 200 GeV…
has closed strangeness
– Canonical Formalism predicts no enhancement…
– Sits between Kaon and Lambda values at 200 GeV...
Also can be described by:
62 GeV B = 1.2
200 GeV B = 2.9
arXiv:0810.4979v1
QuickTime™ and a decompressor
are needed to see this picture.
STAR
7/13
Bulk strangeness productionWhat does this scaling mean? Proposed by F. Becattini and J. Manninen to be indicative of
core-corona effects (arXiv:0811.3766v1)
– Participants with one collision = corona
– Participants with multiple collisions = core
Strangeness equilibrated in core
– B particle density
Strangeness p+p like in corona
Alternative core-core model EPOS approximately reproduces scaling
– As does AMPT (string+rescattering)….
STAR
8/13
Mid-pT spectraBaryon/meson ratios at Au+Au 200 GeV…
Strange baryon/meson anomalies established at STAR
– Quark coalescence? Mid-pT baryon production
preferable to meson production
Coalescence models reproduce qualitative features of ratios
– p/ /K0
S
/
Predict turnover…
– Fail to get pT position right…
Sarah Blyth, Quark Matter 2006
STAR
9/13
Mid-pT spectraBaryon/meson ratios at 62 GeV…
New Cu+Cu 62 GeV data…
High strange baryon/meson ratios observed for both systems– Coalescence occuring at lower energy?
STAR Preliminary
STAR
10/13
Mid-pT spectraComparisons to EPOS…
EPOS Core
– Flow induced, gives higher mass particles pT kick at mid-pT
EPOS Corona
– Dominates production at high-pT
62 GeV
200 GeV
STAR Preliminary
Energy =
Are high baryon/meson ratios unique to coalescence?
STAR
11/13
Hard processes and strangenessRAA of identifed particles…
New high-pT p+p and Au+Au 200 GeV data…
– p+p shown Yichun Xu’s talk in Ridge Phenomena and Jet Flavor Conversion
Parton flavor conversion prediction (Phys. Rev. C77 (2008) 054902)
– Hard scattered partons interact with medium, convert flavour
– Boosts kaon RAArelative to pion RAA
Data consistent with conversion scenario…
STAR preliminary
pT (GeV/c)
STAR
12/13
Hard processes and strangenessRAA vs. system size… Measure integrated RAA for pT > 5.5 GeV/c
– <pT> ~ 6.2 GeV/c
Ratio
– Above one for all centralities
– Strangeness enhancement at high-pT!
In particular, RAA (K) > RAA () for Au+Au where <Npart> ~ 20
– Does parton flavor conversion happen in small systems?
– Can we dismiss the Cronin effect?
– Do we have to push higher in pT for parton conversion searches?
New high-pT p+p and Au+Au 200 GeV data…
STAR
13/13
Summary Bulk strangeness production
– Enhancement for many particles appears to depend on fraction of participants that undergo multiple collisions
Expected in core-corona scenario Also reproduced by AMPT
Mid-pT spectra– Coalescence typically describes trends– Core-corona+flow can also explain strange high baryon/meson ratios
Hard processes and strangeness– Hint of jet conversions in central Au+Au
Kaon RAA higher than pion RAA – Also applies to small systems
Can jet conversions happen there also? Could other effects contribute?
STAR
14/13
Hard processes and strangenessFlavor changing…
Prediction: hard scattered partons interact with medium, convert flavour– Boosts Kaon RAArelative to non-conversion scenario
Kaon RAA factor of two higher at RHIC– Excellent PID for K0
S at STAR…– LHC predicts modest increase
STAR
15/13
Mid-pT spectraQuark coalescence in AMPT…
Phys. Rev. C 78 (2008) 034907
Use particle ratios and constituent quark scaling
– Extract shape of strange and up/down quark spectra
Use shapes as input for AMPT’s quark distributions
– Run in coalescence mode…
Good description of , and spectra in central Au+Au 200 GeV collisions
– Shows quark spectra shapes can be extracted accurately…