Motivations - HADES C+C 1 AGeV, 2 AGeV - measured excess: beam energy dependence p+p, d+p 1.25 (A)GeV - Studies of NN-Bremsstrahlung and  Dalitz decay.

Slides:



Advertisements
Similar presentations
Di-electron Continuum at PHENIX Yorito Yamaguchi for the PHENIX collaboration CNS, University of Tokyo Rencontres de Moriond - QCD and High Energy Interactions.
Advertisements

Direct virtual photon production in Au+Au collision at 200 GeV at STAR Bingchu Huang for the STAR collaboration Brookhaven National Laboratory Aug
Bingchu Huang, USTC/BNL 1 Bingchu Huang (for STAR Collaboration) University of Science and Technology of China (USTC) Brookhaven National Laboratory (BNL)
Summary from lecture I Meson line shape modifications seen in p+A/  +A reactions: 1.E325/KEK : downward  mass shift (~ 9%) 2.E325/KEK: downward  mass.
1 Measurement of phi and Misaki Ouchida f or the PHENIX Collaboration Hiroshima University What is expected? Hadron suppression C.S.R.
Dielectrons from HADES to CBM Bratislava (SAS, PI), Catania (INFN - LNS), Cracow (Univ.), Darmstadt,(GSI), Dresden (FZR), Dubna (JINR), Frankfurt (Univ.),Giessen.
Direct-Photon Production in PHENIX Oliver Zaudtke for the Collaboration Winter Workshop on Nuclear Dynamics 2006.
Studying hadron properties in baryonic matter with HADES „Nuclear matter at High densities” Hirschegg Hirschegg P. Salabura.
Search for Thermal Photons in PHENIX - Torsten Dahms - Stony Brook University 23 rd Winter Workshop On Nuclear Dynamics February 13, 2007.
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
SQM2006, 03/27/2006Haibin Zhang1 Heavy Flavor Measurements at STAR Haibin Zhang Brookhaven National Laboratory for the STAR Collaboration.
Christian Müntz (Univ. Frankfurt) for the HADES Collaboration, CPOD Challenges in Physics & Instrumentation Results from Heavy Ion and Elementary.
Vector meson study for the CBM experiment at FAIR/GSI Anna Kiseleva GSI Germany, PNPI Russia   Motivation   The muon detection system of CBM   Vector.
RICH PylosR. Gernhäuser (TU-München) The HADES RICH High Acceptance Di-Electron Spectrometer The HADES Spectrometer Special requirements RICH setup.
C B M Di-electron background studies and first results using compact RICH CBM Collaboration Meeting, 27 September 2007, Dresden Di-electron background.
Di-electron pair reconstruction CBM Collaboration Meeting, 28 February 2008, GSI-Darmstadt Di-electron pair reconstruction Tetyana Galatyuk GSI-Darmstadt.
T.C. Jude D.I. Glazier, D.P. Watts The University of Edinburgh Strangeness Photoproduction At Threshold Energies.
Yuriy Riabov QM2006 Shanghai Nov.19, Measurement of the leptonic and hadronic decays of  and ω mesons at RHIC by PHENIX Yuriy Riabov for the Collaboration.
PHENIX Fig1. Phase diagram Subtracted background Subtracted background Red point : foreground Blue point : background Low-mass vector mesons (ω,ρ,φ) ~
Victor Ryabov, PNPI SQM 2007 Levoca Jun.27, Measurement of the light mesons with the PHENIX experiment at RHIC Victor Riabov for the Collaboration.
1 Исследование образования электрон-позитронных пар в нуклон-нуклонных взаимодействиях на установке HADES Кирилл Лапидус, ИЯИ РАН Научная сессия-конференция.
Probing resonance matter with HADES „” „EMMI Workshop and XXVI Max Born Symposium” Wrocław Wrocław P. Salabura Jagiellonian University/GSI.
Wolfgang Kühn, Universität Giessen Recent Results from HADES Physics Motivation Low mass lepton pair enhancements SPS and DLS data The HADES detector at.
Dielectron production in C+C collisions at 2AGeV with HADES Jochen Markert For the HADES Collaboration.
Single Electron Measurements at RHIC-PHENIX T. Hachiya Hiroshima University For the PHENIX Collaboration.
Study of hadron properties in cold nuclear matter with HADES Pavel Tlustý, Nuclear Physics Institute, Řež, Czech Republic for the HADES Collaboration ,
ENHANCED DIRECT PHOTON PRODUCTION IN 200 GEV AU+AU IN PHENIX Stefan Bathe for PHENIX, WWND 2009.
HADES coll. meeting, Oct. 31, 2007 Charged pion production in C+C at 1 and 2 A GeV results of data analysis from experiments NOV02 and AUG04 Jehad Mousa.
Charmonium feasibility study F. Guber, E. Karpechev, A.Kurepin, A. Maevskaia Institute for Nuclear Research RAS, Moscow CBM collaboration meeting 11 February.
V.L. Kashevarov. Crystal Collaboration Meeting, Mainz, September 2008 Photoproduction of    on protons ► Introduction ► Data analysis.
Di-electron measurements with HADES at SIS100 Motivation Motivation HADES di-electron results (SIS 18) - summary HADES di-electron results (SIS 18) - summary.
G. Musulmanbekov, K. Gudima, D.Dryablov, V.Geger, E.Litvinenko, V.Voronyuk, M.Kapishin, A.Zinchenko, V.Vasendina Physics Priorities at NICA/MPD.
Introduction to theory session main issues to be discussed during this session.
HADES versus DLS: no puzzle anymore ! Elena Bratkovskaya , Workshop ‚Bremsstrahlung in dilepton production‘ GSI, Darmstadt.
1 Pion production in np collisions at 1.25AGeV A.Kurilkin, P.Kurilkin, V.Ladygin, A.Ierusalimov, T.Vasiliev, LHEP-JINR, Dubna, Russia For the HADES collaboration.
Λ and Σ photoproduction on the neutron Pawel Nadel-Turonski The George Washington University for the CLAS Collaboration.
Measurements of thermal photons in heavy ion collisions with PHENIX - Torsten Dahms - Stony Brook University February 8 th, 2008 Real photons at low p.
03/13/2012Moriond QCD and High Energy Interactions, Mar Di-lepton production at STAR Outline: Motivation and Introduction Recent results from STAR.
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.
Study of b quark contributions to non-photonic electron yields by azimuthal angular correlations between non-photonic electrons and hadrons Shingo Sakai.
NSTAR2011, Jefferson Lab, USA May 17-20, 2011 Mitglied der Helmholtz-Gemeinschaft Tamer Tolba for the WASA-at-COSY collaboration Institut für Kernphysik.
JPS/DNPY. Akiba Single Electron Spectra from Au+Au collisions at RHIC Y. Akiba (KEK) for PHENIX Collaboration.
28/8/2006NN2006, Rio de Janeiro August 28 - September 1, Dielectron production in C+C collisions with HADES Pavel Tlusty, NPI Rez for the Hades.
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
Outline Motivation The STAR/EMC detector Analysis procedure Results Final remarks.
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - State University of New York at Stony Brook for the PHENIX.
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.
XLVII Int. Winter Meeting, Bormio, Jan , 2009 CHARGED PION PRODUCTION IN C+C AND Ar+KCl COLLISIONS MEASURED WITH HADES Pavel Tlustý, NPI Řež for.
PHOBOS at RHIC 2000 XIV Symposium of Nuclear Physics Taxco, Mexico January 2001 Edmundo Garcia, University of Maryland.
Christina MarkertHirschegg, Jan 16-22, Resonance Production in Heavy Ion Collisions Christina Markert, Kent State University Resonances in Medium.
Heavy Quark Production in 920GeV Proton Nucleus Interactions Michael Danilov ITEP, Moscow Representing HERA-B Collaboration Outline 1.Detector and data.
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - Master of Arts – Thesis Defense Stony Brook University.
1 Recent Results on J/  Decays Shuangshi FANG Representing BES Collaboration Institute of High Energy Physics, CAS International Conference on QCD and.
Systematic measurement of light vector mesons at RHIC-PHNEIX Yoshihide Nakamiya Hiroshima University, Japan (for the PHENIX Collaboration) Quark Matter.
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Dilepton production in p+p collisions at 3.5 GeV experimental results and their interpretation Anar Rustamov for the HADES collaboration GSI Helmholtzzentrum.
J. Zhao Hard Probe 2012, Cagliari 1, Lawrence Berkeley National Lab, USA 2, Shanghai Institution of Applied Physics, CAS, China Di-electron Production.
PHENIX J/  Measurements at  s = 200A GeV Wei Xie UC. RiverSide For PHENIX Collaboration.
Dielectron Spectroscopy
Highlights from HADES Au+Au collisions at 1.23 AGeV
Exclusive w/h production in pp collisions at Ekin=3.5 GeV with HADES
A heavy-ion experiment at the future facility at GSI
HADES The Baryon-rich Side of the Phase Diagram
Simulation results for the upgraded RICH detector in the HADES experiment. Semen Lebedev1,3, Jürgen Friese2, Claudia Höhne1, Tobias Kunz2, Jochen Markert4.
Dilepton production with HADES
Identified Charged Hadron
HADES at FAIR P. Salabura Jagiellonian University Kraków.
Identified Charged Hadron Production at High pT
Jerzy Pietraszko, HADES at SIS100 - status GSI Darmstadt, Germany
Presentation transcript:

Motivations - HADES C+C 1 AGeV, 2 AGeV - measured excess: beam energy dependence p+p, d+p 1.25 (A)GeV - Studies of NN-Bremsstrahlung and  Dalitz decay - N+N (p+p & d+p) to C+C comparison Dielectron production at 1-2 AGeV with HADES Motivations - HADES C+C 1 AGeV, 2 AGeV - measured excess: beam energy dependence p+p, d+p 1.25 (A)GeV - Studies of NN-Bremsstrahlung and  Dalitz decay - N+N (p+p & d+p) to C+C comparison Witold Przygoda, Jagiellonian University, Cracow, for the HADES Collaboration International Conference on Particles And Nuclei PANIC 2008, Eilat Israel Dan Eilat Hotel Big Blue Hall A 10 Nov 2008

2 The case of moderate beam energies t [fm/c] ≈ 10 fm/c comparatively long life-time...at moderate densities c  fm/c Baryonic matter (pions less than 10%)  t(   > 2) ≈ 10 fm/c In-medium invariant mass reconstruction Combinatorial background reduction Strategy: systematic e + e – spectroscopy in proton, pion and heavy ion induced reactions Goal: learn about radiation from baryonic rich matter Meson production at or below threshold : co-operative processes (i.e. multi step processes) off-shell effects elementary sources not known well (i.e. baryon resonance decays)

3 High Acceptance Di-Electron Spectrometer  Installed at the SIS18 GSI Darmstadt (Germany) Beams: pions, protons, nuclei  Spectrometer with high invariant mass resolution (2% at  /  mass)  Utilizes dedicated second level trigger processors to select rare events before mass storing Geometry Full azimuth, polar angles 18  - 85  ( y = 0 – 2 ) Pair acceptance  0.35 ~ channels, segmented solid or LH 2 targets Side View START 1 m

4 Experimental (production) runs p+p 1.25 GeV (2006) 2.2 GeV (2002) 3.5 GeV (2007) d+p C+C 2.0 AGeV (2002) 1.0 AGeV (2004) 1.25 GeV (2007) Ar+KCl 1.75 GeV (2005) p+Nb 3.5 GeV (2008) p+p „Anomalous” excess of dilepton pairs in 0.15 < M ee < 0.5 GeV/c 2 NN-Bremsstrahlung and  Dalitz decays Vector meson  /  /  production p+p Calibration & verification measurement of rare electromagnetic decays  +p/A Ni+Ni/Au+Au ( ) FUTURE

5 log. z axis ! e-e- e+e+ hadron : lepton suppression ~10 -4 Analysis strategies Single electron analysis 2-dim cuts on RICH rings, Shower, p vs , hit matching track fitting quality e+e- pair analysis close pair cuts opening angle  > 9° e-e-e-e- e+e+e+e+  M inv = p1p1 p2p2 Target RICH HADRONS Momentum vs velocity (β) dE/dx in MDC & TOF LEPTONS Corrections for detector and reconstruction efficiencies  acceptance & reconstruction efficiency filters available

6 PLUTO event generator (HADES Collaboration) COCKTAIL A (thermal freezout)  0 and  well known  from m T scaling 1 and 2 AGeV - mass spectrum eff. corrected Phys.Rev.Lett. 98 (2007)  (M ee )~9% at M ee ~0.8 GeV/c 2 Phys. Lett. B 663 (2008) 43 in HADES acceptance syst. error (21%) syst. error (27%) COCKTAIL B : COCKTAIL A + short lived  0 and  NORMALIZATION I. Fröhlich et al. (2007) arXiv: [nucl-ex]

7 C+C – pair excess (Y exc ) : scaling with E beam Excess function F(energy) -  region TAPS 0.3(  sys) F(2.0) = 1.9 ± 0.2(stat) ± 0.3(sys) ± 0.3(  sys) 2.0(  sys) F(1.0) = 6.8 ± 0.6(stat) ± 1.3(sys) ± 2.0(  sys)  HADES and DLS resuls agree  Y exc scales with E beam like pion production R. Averbeck et al. Z. Phys. A 359 (1997) 65 R. Holzmann et al. Phys. Rev. C 56 (1997) R2920 TAPS Collaboration

8 N-N Brehmsstrahlung +  Dalitz decay Collection of results on NN-Bremsstrahlung from: New OBE calculations NN Bremsstrahlung is larger than predicted by SPA pp Bremstrahlung is smaller than pn at ~1 AGeV Kaptari & Kämpfer Nucl. Phys. A 764 (2006) 338 (thick line: propagator of nucleon / baryon resonance) E.L. Bratkovskaya et al. Nucl. Phys. A 807 (2008) 214

9 Recent (>2006) transport calculations M. Thomère et al. Phys. Rev. C 75 (2007) E.L. Bratkovskaya et al. Nucl. Phys. A 807 (2008) 214 need more constrains from measured NN collisions IQMD HSD C+C 2 AGeV NN-Bremsstrahlung adjusted to OBE-calculations ”old” SPA NN-Bremsstrahlung …do they unambiguously explain dilepton excess? BRoBUU H.W. Barz, B. Kämpfer, Gy. Wolf, M. Zetenyi (2006) nucl-th/ v3 see also

GeV -  Dalitz decay  Dalitz decay e+e+ ++ e-e- p Time-like  - N transition  branching ratio?  electromagnetic form factors? q 2 = M 2 inv (e + e - ) = M  * 2 > 0 ** Krivoruchenko et al. Phys. Rev. D 65 (2001) grey band Iachello VMD QED a) parameterization a-la Kaptari & Kämpfer + NN Final State Interactions + isotropic  * production preliminary Q. Wan & F. Iachello Int. J. Mod. Phys. A 20 (2005) 1846 b)  Dalitz decay : a-la Krivoruchenko (QED) + VMD form-factor PLUTO calculations

AGeV – quasifree p-n collisions selection of np reactions by measurement of spectator proton in Forward Wall spectator " tag " Mult.  1 FW (0.5  –7  ) contribution of p+p in p+n after FW selection less than 12% (M M  0 ) a) sum of np-Bremsstrahlung a-la Kaptari & Kämpfer,  and  Dalitz decays b) Fermi momentum of nucleon in deuterium from N-N Bonn potential deuteron spectator proton proton reaction proton e + e – X FSI preliminary PLUTO calculations

12 1 AGeV – pp & 1.25 Dielectron spectrum from C+C: superposition of NN collisions! No indications for in-medium effects (at least for C+C) spectra normalized to  0 measured in C+C and NN 1 AGeV /A part = 0.06 ± (A)GeV

13 Summary 12 C and 2 AGeV analyzed and published –DLS data 1.04 AGeV) confirmed –dilepton pair excess in  region (0.15 GeV/c 2 < M ee < 0.5 GeV/c 2 ) observed –excess seems to scale with energy beam like pion production –new OBE calculations: significantly higher pn-Bremsstrahlung contribution –various transport models describe data although with different scenarios p+p and 1.25 (A)GeV –elementary reactions in order to measure  and NN-Bremsstrahlung –problems with description of pp and pn data –normalized spectra of C+C and pp+pn agree (not due to in-medium effects) –more data to theoretical models in elementary dilepton production channels Vector meson investigation in HADES 3.5 GeV analysis on-going 3.5 GeV measurement just completed 1.75 AGeV analysis almost completed Plans –heavy systems (Ni+Ni, Au+Au) and pion-N/A after HADES upgrade (2009) –further program at FAIR (up to 8 AGeV) anticipated

14 HADES Collaboration