Quark Matter 2006 November 14-20, Shanghai NA60 results on the  spectral function in Indium-Indium collisions J. Seixas NA60 Collaboration.

Slides:



Advertisements
Similar presentations
The NA60 Experiment Readout Architecture M.Floris, D.Marras, G.Usai, A.David, P.Rosinsky, H.Ohnishi for the NA60 Collaboration 13 th IEEE- NPSS Real Time.
Advertisements

1 Gianluca Usai – University of Cagliari and INFN Electromagnetic Probes of Strongly interacting Matter in ECT* Trento - 23/05/2013 The QCD phase diagram.
 production in proton-nucleus and indium-indium collisions Michele Floris University and INFN, Cagliari, Italy. on behalf of the NA60 Collaboration ISMD.
Yorito Yamaguchi For the PHENIX collaboration CNS, University of Tokyo 10/14/2008ATHIC2008 1/13.
NA60 results on charm and intermediate mass dimuon production in In-In 158 GeV/A collisions R. Shahoyan, IST (Lisbon) on behalf of the NA60 collaboration.
Di-electron Continuum at PHENIX Yorito Yamaguchi for the PHENIX collaboration CNS, University of Tokyo Rencontres de Moriond - QCD and High Energy Interactions.
1 J/ production in In-In and p-A collisions Gianluca Usai University of Cagliari and INFN Introduction Centrality dependence of J/ suppression in In-In.
S. Damjanovic, Bielefeld 13 December First measurement of the  spectral function in high-energy nuclear collisions Sanja Damjanovic NA60 Collaboration.
1 Measurement of phi and Misaki Ouchida f or the PHENIX Collaboration Hiroshima University What is expected? Hadron suppression C.S.R.
06/10/2008Alessandro De Falco (NA60) SQM081 Highlights from the NA60 Experiment Alessandro De Falco University and INFN Cagliari on behalf of the NA60.
The Beamscope Cryogenic Silicon Beam Tracker of NA60 Peter Rosinský, Bratislava/CERN Vertex ’2002 workshop.
Source Dynamics from Deuteron and Anti-deuteron Measurements in 200 GeV Au+Au Collisions Hugo E Valle Vanderbilt University (For the PHENIX Collaboration)
1 The CMS Heavy Ion Program Michael Murray Kansas.
J/  production in In-In collisions at SPS energies Philippe Pillot — IPN Lyon for the NA60 Collaboration work 2005 June 16–20   Outline: Reminder.
Open charm and charmonium production in p-A collisions at the CERN SPS E. Scomparin (INFN – Torino, Italy), NA60 collaboration Introduction Charmonium.
Charm and intermediate mass dimuons in In+In collisions R. Shahoyan, IST (Lisbon) on behalf of the NA60 collaboration Quark Matter 2005, Budapest Motivation.
H.J.Specht, Erice 2012 Concluding remarks on NA60 (and beyond) Erice, 20 September 2012 Hans J. Specht Physikalisches Institut Universität Heidelberg 1.
Thermal dileptons from NA60 and possible future opportunities at SPS Introduction “thermal” radiation Experimental Challenges State of the art experiment.
I. Ravinovich Di-electron measurements with the Hadron Blind Detector in the PHENIX experiment at RHIC Ilia Ravinovich for the PHENIX Collaboration Weizmann.
QM2006 Shanghai, China 1 High-p T Identified Hadron Production in Au+Au and Cu+Cu Collisions at RHIC-PHENIX Masahiro Konno (Univ. of Tsukuba) for the PHENIX.
Jornadas LIP 2008 – Pedro Ramalhete. 17 m hadron absorber vertex region 8 MWPCs 4 trigger hodoscopes toroidal magnet dipole magnet hadron absorber targets.
Single Electron Measurements at RHIC-PHENIX T. Hachiya Hiroshima University For the PHENIX Collaboration.
Experiments on Lepton Pairs Past, Present, Future ECT* Trento, May 20-24, 2013 Hans J. Specht Physikalisches Institut Universität Heidelberg H.J.Specht,
S. Damjanovic, QM2005, 4-9 August, Budapest1 First measurement of the  spectral function in high-energy nuclear collisions Sanja Damjanovic on behalf.
1 Roberta Arnaldi INFN Torino (Italy) on behalf of the NA60 Collaboration J/  production in Indium-Indium collisions: new results from NA60 Introduction.
S. Damjanovic, Quark Matter Thermal dileptons at SPS energies Sanja Damjanovic NA60 Collaboration Quark Matter 2008, Jaipur.
September 6, 2001Heavy ion physics at CERN after 2000 and before LHC 1 E. Scomparin, INFN-Torino (Italy) NA60 collaboration International Workshop on the.
Roberta Arnaldi — INFN Torino for the NA60 Collaboration J/  production in Indium-Indium collisions: the NA60 experiment Hard Probes 2004, 4-10 Nov
Measurements of thermal photons in heavy ion collisions with PHENIX - Torsten Dahms - Stony Brook University February 8 th, 2008 Real photons at low p.
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
Ralf Averbeck Stony Brook University Hot Quarks 2004 Taos, New Mexico, July 19-24, 2004 for the Collaboration Open Heavy Flavor Measurements with PHENIX.
NA60: dimuon and charm production in p-A and In-In collisions 1 NA60: dimuon and charm production in p-A and In-In collisions at the CERN SPS Introduction.
Dilepton Radiation Measured in PHENIX probing the Strongly Interacting Matter Created at RHIC Y. Akiba (RIKEN Nishina Center) for PHENIX Collaboration.
1 Nuclear modification and elliptic flow measurements for  mesons at  s NN = 200 GeV d+Au and Au+Au collisions by PHENIX Dipali Pal for the PHENIX collaboration.
SQM 2003, Atlantic Beach, NC, USAC. Oppedisano1 Chiara Oppedisano for the NA60 Collaboration Study of prompt dimuon and charm production with proton and.
Muon detection in NA60  Experiment setup and operation principle  Coping with background R.Shahoyan, IST (Lisbon)
 production in p-A and In-In collisions Motivation Apparatus Collected data Results for     Ongoing work for    KK Alessandro De Falco – University.
1 J/, Charm and intermediate mass dimuons in Indium-Indium collisions Hiroaki Ohnishi, RIKEN/JAPAN For the NA60 collaboration XXXV International Symposium.
Dimuon measurements with NA60 Introduction NA60 physics results Low-mass dimuons J/  suppression Future developments International workshop The physics.
JPS/DNPY. Akiba Single Electron Spectra from Au+Au collisions at RHIC Y. Akiba (KEK) for PHENIX Collaboration.
Jeffery T. Mitchell (BNL) – Quark Matter The Evolution of Correlation Functions from Low to High p T : From HBT to Jets Quark Matter 2005 Jeffery.
4/12/05 -Xiaojian Zhang, 1 UIUC paper review Introduction to Bc Event selection The blind analysis The final result The systematic error.
1 - Onset of deconfinement NA60+ - Existence (or non existence) of QCD critical point - Chiral symmetry restoration  Measuring dimuons at different energies.
January 13, 2004A. Cherlin1 Preliminary results from the 2000 run of CERES on low-mass e + e - pair production in Pb-Au collisions at 158 A GeV A. Cherlin.
PHENIX dileptons Thomas K. Hemmick Stony Brook University.
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - Master of Arts – Thesis Defense Stony Brook University.
05/23/14Lijuan Ruan (BNL), Quark Matter The low and intermediate mass dilepton and photon results Outline: Introduction New results on dileptons.
The NA60 experiment at the CERN SPS “Production of open charm and prompt dimuons in collisions of proton and heavy ion beams on nuclear targets” Results.
Low Mass Vector Mesons Nuclear Modification Factors in d+Au 200GeV Lei Guo Los Alamos National Laboratory PHENIX Collaboration.
1 J/ production in p-A collisions at 158 and 400 GeV: results from the NA60 experiment P. Cortese (Università del Piemonte Orientale – Alessandria and.
Measurements of low pT direct photons in PHENIX Yorito Yamaguchi for the PHENIX collaboration CNS, University of Tokyo 04/11/2008WWND South Padre.
Upsilon production and μ-tagged jets in DØ Horst D. Wahl Florida State University (DØ collaboration) 29 April 2005 DIS April to 1 May 2005 Madison.
Dimuon Measurements by NA60 NA60 overview Charmonium production: J/  Intermediate mass dimuons and open charm m T distribution from dimuons Summary Axel.
Thermal Dimuon Emission in In-In at the CERN SPS Michele Floris for the NA60 Collaboration University and INFN, Cagliari, Italy.
Latest results from NA60 P. Cortese for the NA60 Collaboration Università del Piemonte orientale – Alessandria and INFN Europhysics Conference on High.
 Meson Production in In-In Collisions and Highlights from NA60 Michele Floris 1 for the NA60 Collaboration Strangeness in Quark Matter University.
Di-electron elliptic flow in
Bjorn Lenkeit, CERN-EP on behalf of the NA60 Coll. Moriond, March 2001
High-pT Identified Hadron Production in Au+Au and Cu+Cu Collisions
NA60 results on quarkonia
The NA60 experiment at the CERN SPS
Resonances production from the NA60 experiment
The NA60 experiment Reproducing in the lab the early Universe conditions: a plasma of deconfined quarks and gluons (QGP) Third generation experiment which.
Introduction Data analysis Differential distributions (xF,pT)
New results from NA60.
Quarkonium production in ALICE
J/ production in In-In and p-A collisions
Thermal dimuons and f meson production in In-In collisions at the SPS
Highlights from NA60 experiment
High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions
Presentation transcript:

Quark Matter 2006 November 14-20, Shanghai NA60 results on the  spectral function in Indium-Indium collisions J. Seixas NA60 Collaboration

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 2 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Conclusions

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 3 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Conclusions

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 4 Origin of muons can be accurately determined Improved dimuon mass resolution Matching in coordinate and momentum space or ! Measuring dimuons in NA60: concept hadron absorber Muon Other and trackingMuon trigger ACM magnet Iron wall NA50 spectrometer 2.5 T dipole magnet targets beam tracker vertex tracker  40 cm >10 m prompt displaced

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 5 Event sample  5-week long run in Oct.–Nov  Indium beam of 158 GeV/nucleon ~ 4 × ions delivered in total ~ 230 million dimuon triggers on tape  Present analysis: ~1/2 of total data

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 6 Main steps of the data analysis  Reconstruction of the event vertex within the segmented target  Matching of tracks from muon spectrometer and silicon vertex telescope  Assessment of fake matches (incorrect match between tracks in the muon spectrometer and silicon vertex telescope) by overlay MC and/or event mixing: agreement ~5%  Assessment of combinatorial background (pairing of uncorrelated muon pairs from  and K decays) by event mixing: accuracy ~1%

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 7 Mass spectrum  Net data sample: events  Fakes / CB < 10 %  ω and  peaks clearly visible in dilepton channel; even μμ seen  Mass resolution: 23 MeV at the  position  Progress over CERES: statistics: factor >1000 resolution: factor 2-3 ω  

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 8 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Comparison to theoretical models

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 9 Isolation of the excess   and  : fix yields such as to get, after subtraction, a smooth underlying continuum   : (  ) set upper limit, defined by “saturating” the measured yield in the mass region close to 0.2 GeV/c 2 (lower limit for excess). (  ) use yield measured for p T > 1.4 GeV/c difference spectrum robust to mistakes on the 10% level, since the consequences of such mistakes are Highly localized.

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 10 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Conclusions

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 11 Excess mass spectra for 12 centrality bins Cocktail  from /=1.2 Excess always centered at nominal -pole, while width increases

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 12 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Conclusions

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 13 Shape modification vs. centrality Divide region around peak in 3 windows labeled L, C and U: Peak/ρ Ratio Continuum/ρ “Peak” decreases with respect to cocktail ρ by ~2 from first to last point Change in trend for dN ch /dy > 100

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 14 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Conclusions

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 15 Comparison to theory [talks by R. Rapp, V. Metag, G. Usai]  Predictions for In-In by Rapp et al. (2003) for = 133, covering all scenarios  Data and predictions as shown, after acceptance filtering, roughly mirror the respective spectral functions, averaged over space-time and momenta.  Theoretical yields normalized to data in mass interval < 0.9 GeV/c 2. Only broadening of  (RW) No mass shift (BR) observed

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 16 Outline  Event sample  Isolation of excess dimuons above hadron decays  Mass spectra  Shape analysis of mass spectra  Comparison to theory  Acceptance-corrected p T spectra  Conclusions

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 17 Strategy for acceptance correction  Reduce 3-dimensional acceptance correction in M-p T -y to a 2-dimensional correction in M-p T, using measured y distribution as an input. Use  for control.  Use slices of m = 0.1 GeV p T = 0.2 GeV  Check behaviour on 3 extended mass windows 0.4<M<0.6 GeV 0.6<M<0.9 GeV 1.0<M<1.4 GeV Subtract charm from the data (based on NA60 IMR results) before acceptance correction

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 18 Rapidity distribution of the excess  Agreement between the three p T bins  Results close to rapidity distribution of  ’s (from NA49 and NA60) for the same √s arb. units

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 19 Excess p T spectra: 3 centrality bins Hardly any centrality dependence BUT Significant mass dependence

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 20 Systematics of low-p T data: Combinatorial background  Enhanced yield at low- p T seen at all centralities, including the peripheral bin  Errors at low p T, due to subtraction of combinatorial background: Enhanced yield at low p T not due to incorrect subtraction of combinatorial background peripheral1% semiperipheral10% semicentral20% central25%

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 21 Excess p T spectra: mass dependence  Since we do not observe any centrality dependence, we sum over centralities and keep dependence in mass  Differential fits to p T spectra: assume locally 1-par. m T scaling (~exp(-m T /T eff )) and use gliding windows of p T =0.8 GeV; get T eff for each bin

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 22 Excess p T spectra: mass dependence Systematic errors: < 15 MeV  -like region hardest  high-mass region softest Different sources in different mass regions Hadronic or partonic?  low T low p T Trend opposite to what expected from radial flow (see )

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 23 Conclusions (Mass spectra)  Pion annihilation seems to be a major contributor to the lepton pair excess at SPS energies  Strong broadening, but no significant mass shift of the intermediate 

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 24 Conclusions (p T spectra)  Strong mass dependence of p T spectra  Spectra behave oposite to expected from radial flow  p T spectra could serve as a handle to disentangle partonic from hadronic sources (breaking parton-hadron duality)

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 25 Lisbon CERN Bern Torino Yerevan Cagliari Lyon Clermont Riken Stony Brook Palaiseau Heidelberg BNL ~ 60 people 13 institutes 8 countries R. Arnaldi, R. Averbeck, K. Banicz, K. Borer, J. Buytaert, J. Castor, B. Chaurand, W. Chen, B. Cheynis, C. Cicalò, A. Colla, P. Cortese, S. Damjanović, A. David, A. de Falco, N. de Marco, A. Devaux, A. Drees, L. Ducroux, H. En’yo, A. Ferretti, M. Floris, P. Force, A. Grigorian, J.Y. Grossiord, N. Guettet, A. Guichard, H. Gulkanian, J. Heuser, M. Keil, L. Kluberg, Z. Li, C. Lourenço, J. Lozano, F. Manso, P. Martins, A. Masoni, A. Neves, H. Ohnishi, C. Oppedisano, P. Parracho, P. Pillot, G. Puddu, E. Radermacher, P. Ramalhete, P. Rosinsky, E. Scomparin, J. Seixas, S. Serci, R. Shahoyan, P. Sonderegger, H.J. Specht, R. Tieulent, E. Tveiten, G. Usai, H. Vardanyan, R. Veenhof and H. Wöhri The NA60 experiment

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 27 Backup

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 28 RMS of total excess  Consistency with shape analysis  Further rise starting at dN ch /dy =100  Bad fit (  2 =3) for linear rise above dN ch /dy=30)

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 29 Different model descriptions Renk/Ruppert

J. Seixas (NA60 Coll.) Quark Matter 2006, Shanghai 30

Systematics of low-p T due to the cocktail subtraction radical (unrealistic) increase of  Dal subtraction  20% decrease of yield in mass window 0.6<M<0.9 enhanced yield at low pt cannot be due to incorrect  subtraction

Fit:0-0.4 GeV Teff=82 MeV Teff=97 MeV Teff=118MeV enhanced yield at low pt even after radical increase (by nearly a factor of 2) of the  Dalitz yield Systematics of low-p T data due to the cocktail subtraction