1 / 27

Strange Particle Ratios on the Near- & Away-Sides of Jets at RHIC

SQM 2007, Levoča, Slovakia. Strange Particle Ratios on the Near- & Away-Sides of Jets at RHIC. Jiaxu Zuo Shanghai Institute of Applied Physics & BNL (For STAR Collaboration). Outline. Motivation Analysis Method Results & Discussions Summary. STAR Au+Au 200GeV Year 2004 Running Data

shay-farmer
Télécharger la présentation

Strange Particle Ratios on the Near- & Away-Sides of Jets at RHIC

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. SQM 2007, Levoča, Slovakia Strange Particle Ratios on the Near- & Away-Sides of Jets at RHIC Jiaxu Zuo Shanghai Institute of Applied Physics & BNL (For STAR Collaboration)

  2. Outline • Motivation • Analysis Method • Results & Discussions • Summary • STAR Au+Au 200GeV Year 2004 Running Data • ~13M Events

  3. pT,trig>2.5 GeV/c pT,ass>1.0 GeV/c 0.6 0.4 0.2 0.0 STAR preliminary Di-hadron correlations pT,trig>4 GeV/c pT,ass>2 GeV/c For high pT: away-side correlation is gone! back-to-back jets are quenched At lower pT: away-side correlations return but they are highly modified with a double bump!? We will try to understand what causes this behavior

  4. Centrality dependence M. Horner, QM06 pT,trig>2.5 GeV/c pT,ass>1.0 GeV/c Singly-peaked -> broadened -> becomes doubly bump What’s the baryon/meson ratio in the near- and away-side peak? What are the anti-baryon-to-baryon ratios? We will measure the ratios to try to understand the source of the correlations in different centralities.

  5. B/M Ratio Intermediate pT STAR preliminary large enhancement of baryon/meson ratio in central Au+Au relative to p+p reaches maximum at pT~3 GeV/c Perhaps related to faster increase with centrality of baryon production from recombination Intermediate pT, Baryon & Meson: Grouping of RCP and v2 ----recombination pictures Can recombination explain particle ratios in the jet cones?

  6. Anti-B/B Ratio Intermediate pT STAR preliminary We can also learn about gluons vs quarks from B/B ratios with the jet correlation. For example: anti-baryons  dominated by gluon jets baryons  mixture of quark and gluon

  7. STAR preliminary Anti-Baryon Density H.D.Liu QM06 • Collisions which containggg, qbar+g or qqbar+gprocesses have higher anti-baryon phase space density • Anti-baryon phase space density from collisions involving a gluon is much higher than those without a gluon H. Liu, Z. Xu nucl-ex/0610035 • From B/B ratios in the correlation • Baryon & Anti-baryon production with Jets • Gluon vs. Quarks with Jets

  8. away-side associated Λ, Λ, K0S parton parton near-side associated trigger hadron Λ, Λ, K0S Trigger-associate correlations • Identified particles correlations & B/M , B/B ratio can provide additional information on: • jet quenching • baryon/meson enhancement at STAR • particle production mechanisms • Di-hadron correlation Away-side shape • We’ll study identified associate particles using • Trigger: Charged hadron, pT>3.0 GeV/c • Associate:KS0, , or (i.e. V0 decay), pT>1.0 GeV/c

  9. Analysis method Step 1:3-D histogram with , , and minv (Trigger-V0 pair) Step 2:Project over a given  range in this talk I show results for -1<<1: (combine jets & some ridge) Step 3: Plot minvvs. Fit the minv distribution  yield dN/d( KS0, , or ) minv    minv • Step 4: Repeat 1 to 3 with mixed events • Step 5: Scale the mixed event background with measured v2 • Subtract off the background • ZYAM (zero-yield at the minimum) • ZYA1 (zero-yield at one)

  10. Hadron_Ks & L+L Correlation 3<pT,trig<6 GeV/c; 1<pT,ass<4 GeV/c • Centrality Dependence • Double bump -> Broadened -> Singly-peaked • The shape consistent with di-hadron correlation central peripheral

  11. Hadron_Ks & L+L Correlation 3<pT,trig<6 GeV/c 1<pT,ass<4 GeV/c • Centrality bin: 10-40% • The yellow band : systematic error • From the line: Left part: near-side Right part: away-side Near-Side Away-Side

  12. STAR Preliminary Baryon to Meson Ratio with Jets • Lambda to Ks Ratio : Away-Side > Near-Side • Anti-Proton to p-Ratio : Away-Side > Near-Side (PHENIX) Both STAR and PHENIX results consistent with larger B/M ratio on the Away-Side than Near-Side.

  13. pT,trig>2.5 GeV/c pT,ass>1.0 GeV/c near 0.6 0.4 0.2 Medium away mach cone 0.0 STAR preliminary near Medium away deflected jets The shape of the ratio • Mach Cone Concept/Calculations • Stoecker, Casalderry-Solana et al; Muller et al.; Ruppert et al., … • Cherenkov RadiationMajumder, Koch, & Wang; Vitev • Jet Deflection (Flow) • Fries; Armesto et al.; Hwa M. Horner, QM06 • Can we learn something about the shape on the away-side? • Sound wave excitation particles maybe slower than the speed of sound (vs=c/3) • For our pT range slower particles would have to be heavy • For production from sound wave excitation the bumps should have mostly heavy particles (+)/KS0 would get large in the bump region

  14. near Medium mach cone away Δ = p/2 Trigger Associate Δ=p Medium B/M Ratio in DFDistribution • A slope at Away-Side? L Slow particle  Double bump KS0 Fast particle  Double bump ?? • B/M ratio: Away-Side seems to increase in the "cone" region - as it maybe for sound wave excitation. • Increased B/M ratio may also be consistent with recombination in high density region of the shock-wave • Error bars too large to get strong conclusions • The same shape in the away-side using v2 background from three different methods • The shape of Baryon to Meson ratio on the away-side seems to be independent of v2 background and background subtraction method. • Perhaps a slope , but error bars are still too large to draw conclusions. L+L/KS0 ???

  15. (B/M)A to (B/M)N double ratio central • (B/M)A to (B/M)N double ratio from central to peripheral • 00-10% &10-40% • Maybe a slope here • 40-80% • Difficult to describe • In the correlation function, • 00-10% &10-40% • There is a double bump and broadened away-side. • 40-80% • There seems to be a single peak. peripheral

  16. Hadron_L &L Correlation 3<pT,trig<6 GeV/c; 1<pT,ass<4 GeV/c • Centrality Dependence • Double bump, Broadened & Singly-peaked • The shape consistent with di-hadron correlation peripheral central

  17. Hadron_L &L Correlation 3<pT,trig<6 GeV/c 1<pT,ass<4 GeV/c Centrality bin: 10-40% • The yellow band: Systematic error. • From the line: Left part: near-side Right part: away-side Near-Side Away-Side

  18. (B/B)A to (B/B)N ratio central • (B/B)A to (B/B)N ratio from central to peripheral • The ratio is around one • Maybe a slope at here, but error bars are still too large to conclude. Why is it a slope?? • Independent of v2 and background subtraction method peripheral

  19. Summary • Measured the Conditional Yields of identified associate particles on the near- and away-side of jets • From central to peripheral : Double bump -> Broadened -> Singly-peaked • Extracted particle ratios on the near and away-side • Systematic errors from v2 and background normalization are large • errors can be reduced with more data (to reduce error on the level of the background) • and better understanding of v2 (to reduce uncertainty on the shape of the background) • Both STAR and PHENIX results consistent with larger B/M ratio on the away-side than near-side • Shape of away-side has been studied • some indication of a slope for B/M and L/L on the away-side (mach-cone? gluon vs. quark? Or others?) • slope of B/M and L/L on the away-side seems to be independent of v2 and background subtraction method Acknowledgments: STAR Collaboration Dr. Paul Sorensen Thanks!!

  20. The Collaboration Shanghai Institue of Applied Physics - Argonne National Laboratory Institute of High Energy Physics - University of Birmingham - Brookhaven National Laboratory - California Institute of Technology - University of California, Berkeley - University of California, Davis - University of California, Los Angeles - University of Illinois at Chicago - Carnegie Mellon University - Creighton University – Nuclear Physics Inst., Academy of Sciences - Laboratory of High Energy Physics - Particle Physics Laboratory - University of Frankfurt - Institute of Physics, Bhubaneswar - Indian Institute of Technology, Mumbai - Indiana University Cyclotron Facility - Institut de Recherches Subatomiques de Strasbourg - University of Jammu - Kent State University - Institute of Modern Physics - Lawrence Berkeley National Laboratory - Massachusetts Institute of Technology - Max-Planck-Institut fuer Physics - Michigan State University - Moscow Engineering Physics Institute - City College of New York - NIKHEF and Utrecht University - Ohio State University - Panjab University - Pennsylvania State University - Institute of High Energy Physics - Purdue University – Pusan National University - University of Rajasthan - Rice University - Instituto de Fisica da Universidade de Sao Paulo - University of Science and Technology of China - SUBATECH - Texas A&M University - University of Texas, Austin - Tsinghua University - Valparaiso University – Variable Energy Cyclotron Centre, Kolkata - Warsaw University of Technology - University of Washington - Wayne State University - Institute of Particle Physics - Yale University - University of Zagreb -UNICAMP

  21. Backup

  22. V0 reconstruction V0s from UCLA/LBL picoDsts

  23. Fragmentation and energy loss - near-side after v2 subtraction jet+ridge Dj  trigger  jet ridge  ridge Di-hadron correlations pTtrig=3-6 GeV/c, 1.5 GeV/c <pTassoc< pTtrig h-h jet ridge a.u.  Dh Df v2 + away-side peak Au+Au central @ 200 GeV Au+Au: long-range Dh correlations at near side (“the ridge”) Lesson: The near-side jet does interact with the medium

  24. Weight average flow: Ks, L & Hadron v2 • Final results background: Average v2 • Ks and L: v2{EP} & v2{LYZ} • Charged Hadron: v2{EP} & v2{4} • A part of systematic errors will be calculated by the v2{EP} & v2{LYZ}, v2{4} • Background:V0 & Hadron v2 • Background function:B()=b0(1+2<v2A*v2B>cos(2)) • V0 LYZ v2:pt [1,4] • Hadron v2{4}:pt [3.2,6.5] v2{4} & v2{EP} Phys. Rev. C 72 (2005) 014904 v2{LYZ} paper in preparation

  25. all events First minimum of |G|2 determines r0 average over  Lee-Yang Zeroes method • Lee-Yang Zeroes method is less biased by non-flow correlation. Nucl. Phy. A 727 (2003) 373-426 • Sum generating function: • Flow vector projection into arbitrary angel . • Generating function for a given . • Integrated flow: • From the first minimum r0 • Differential flow all particles in all events average over  removes acceptance effects

  26. Same Event & v2 Background STAR preliminary for these plots, efficiency correction not applied

  27. Ratio vs.Df • B/B Ratio at Near-Side • B/B Ratio vs.Df at Away-Side • B/M Ratio at Near-Side • B/M Ratio vs.Df at Away-Side

More Related