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Measurements of dileptons with the CBM-Experiment at FAIR Claudia Höhne, University Giessen CBM collaboration.

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Presentation on theme: "Measurements of dileptons with the CBM-Experiment at FAIR Claudia Höhne, University Giessen CBM collaboration."— Presentation transcript:

1 Measurements of dileptons with the CBM-Experiment at FAIR Claudia Höhne, University Giessen CBM collaboration

2 Claudia Höhne Quark Matter, Darmstadt, May 20142 Outline Introduction & motivation Detector concept of CBM overall concept challenges of the dilepton measurement: electrons – muons Simulations feasibility studies for di-electrons and di-muons background analysis Detector development Summary and Outlook Related Posters RICH detector development: M-09, M-10, M-11 MUCH detector development: M-03 Di-Electron simulations: G-18

3 Claudia Höhne Quark Matter, Darmstadt, May 20143 The QCD diagram at high  B phase diagram at high  B ? quarkyonic phase? phase transition(s)? critical point/ triple point? need for high precision data including rare probes! Electromagnetic probes! Field driven by experimental data! [A. Andronic et al., arXiv:0911.4806 ]

4 Claudia Höhne Quark Matter, Darmstadt, May 2014 Physics case (I) 4 [HADES, Phys.Rev. C84 (2011) 014902] [CERES: Phys.Lett.B 666, 425 (2008)] [calculations: H. v. Hees, R. Rapp, Nucl.Phys.A806:339,2008] Relevance of HADES data for understanding high-energy LMVM spectra: strength of dilepton yield at low masses is due to coupling to baryons! Dilepton yield at highest net-baryon densities?

5 Claudia Höhne Quark Matter, Darmstadt, May 2014 Physics case (II) 5 [NA60, Eur.Phys.J. C61 (2009) 711-720]

6 Claudia Höhne Quark Matter, Darmstadt, May 2014 Physics case (III) 6 [ALICE, Phys.Rev.Lett. 109 (2012) 072301] [CBM Physics Book] ? quark like (pre-)hadron like

7 Claudia Höhne Quark Matter, Darmstadt, May 20147 Dileptons at FAIR - the aim no ρ,ω,φ → e + e - (  +  - ) measurement between 2 and 40 AGeV no J/ψ → e + e - (μ + μ - ) measurement below 158 AGeV Study EM radiation (+ heavy flavor) in baryon dominated matter at moderate temperature as accessible by FAIR! Photons: access to early temperatures Low-mass vector mesons: in- medium properties of  Intermediate range: acces to fireball radiation J/  : charm as a probe for dense baryonic matter [A. Drees]

8 Claudia Höhne Quark Matter, Darmstadt, May 20148 The Facility for Antiproton and Ion Research CBM and HADES at SIS-100 and SIS-300 systematic exploration of baryon dominated, high density matter in A+A collisions from 2 – 45 AGeV beam energy with 2nd generation experiments HADES: Au+Au collisions 2-4 AGeV, low material budget, 20°-85° polar angle CBM: Au+Au collisions 4-35 AGeV, larger material budget, 2.5°-25° polar angle

9 Claudia Höhne Quark Matter, Darmstadt, May 20149 CBM @ SIS-100 & SIS-300 Beamp lab, max √s NN, max heavy ions (Au)11A GeV4.7 GeV light ions (Z/A = 0.5)14A GeV5.3 GeV protons29 GeV7.5 GeV The first years of CBM operation will be at SIS-100 with a start setup Beamp lab, max √s NN, max heavy ions (Au)35A GeV8.2 GeV medium ions (In) (Cu) 38A GeV 41A GeV 8.5 GeV 8.9 GeV light ions (Z/A = 0.5)45A GeV9.3 GeV protons90 GeV13 GeV CBM at SIS-300 …. at interaction rates up to 10 MHz (J/  )

10 Claudia Höhne Quark Matter, Darmstadt, May 201410 CBM – detector concept fixed target experiment, "medium" energies → large solid angle to be covered high rate, multipurpose detector including open charm reconstruction → fast, excellent tracking based on silicon pixel and strip detectors directly behind the target and inside a magnetic field → add particle identification downstream (leptons, hadrons) beam magnet (MVD)+STS RICH / MUCH (TRD) TOF drives layout

11 Claudia Höhne Quark Matter, Darmstadt, May 2014 The CBM experiment 11 HADES MVD + STS RICH TRD PSD EMC (park. pos.) Muon detector (parking position) dipole magnet Tracking, momentum, V 0 : MVD+STS+dipole magnet Event characterization: PSD Hadron id: TOF Lepton id: RICH+TRD or MUCH ,  0 : EMC High speed DAQ & trigger TOF SIS 100 setup

12 Claudia Höhne Quark Matter, Darmstadt, May 2014 Simulation input 12 CBMROOT framework, GEANT3 Background: UrQMD v. 3.3 Signal: PLUTO with multiplicities from HSD (semi-)realistic detector descriptions Muons:  STS: realistic detector response, clustering, material from cables…  MUCH: realistic detector response, clustering Electrons:  STS: realistic detector response, clustering, material from cables…  RICH: realistic detector response  TRD: semirealistic detector response (hit smearing)  TOF: semirealistic detector response (hit smearing)

13 Claudia Höhne Quark Matter, Darmstadt, May 2014 Muon detection system: MUCH 13 LMVM @ SIS100 + ToF LMVM @ SIS300 + ToF ID after hadron absorber with intermediate tracking layers major combinatorical background from ,K decays into , punch through of hadrons and track mismatches → use excellent tracking to reject ,K decays in the STS 60 C + 20 Fe + 20 Fe + 30 Fe + 35 Fe + 100 Fe (cm) 30 cm gap between 2 absorbers

14 Claudia Höhne Quark Matter, Darmstadt, May 2014 Background - muons 14 Particles identified as muons = reconstructed after MUCH (25 AGeV central Au+Au) Total number allows for a trigger also for LMVM min. 14 MuCh hits LMVM setup (no TOF) J/  setup (no TOF) min. 17 MuCh hits (70%)

15 Claudia Höhne Quark Matter, Darmstadt, May 2014 Decay muons 15 Background dominated by decay muons Vertex-z distribution of reconstructed  tracks in STS/ MUCH: Successful reduction of decay muons by tracking cuts!  -ID in STS  -ID in MUCH

16 Claudia Höhne Quark Matter, Darmstadt, May 2014 Invariant mass spectra – muons 16 Shown: central (b=0fm) Au+Au collisions at 25 AGeV Mass resolution: 12 MeV (  ) and 29 MeV (J/  ) only due to momentum determination in STS LMVM spectra for SIS100 show similar quality J/  in central pAu at 30GeV with superb S/B ratio S/B 2  = 1.68 J/     

17 Claudia Höhne Quark Matter, Darmstadt, May 2014 Electron ID – RICH + TRD 17 identification: RICH, TRD and TOF – no e-ID in front of B-field clean electron identification (  suppression ≥ 10 4 ) major combinatorial background from physical sources  -conversions in target and STS,  0 Dalitz decays → use excellent tracking and topological cuts for bg rejection (LMVM) → use (segmented) target with thin (0.1% int. length) foil(s) 13% Track Segment Electron Track e ± from π 0 + electron track = true pair

18 Claudia Höhne Quark Matter, Darmstadt, May 201418 Background contributions – LMVM central (b=0fm) Au+Au collisions at 25 AGeV, 200k events e± tracks contributing per event: 0.14 from  0 -Dalitz decay (60%) 0.07 from  -conversion (29%) 0.007 misidentified  ±  0.016 secondary e ± (7%) Related Poster Di-Electron simulations: G-18 γ-γ – e + and e - from different γ-conversions π 0 -π 0 – e + and e - from different π 0 -Dalitz decays o. - e ± from other sources including misidentification

19 Claudia Höhne Quark Matter, Darmstadt, May 2014 Invariant mass spectra - electrons 19 1.6 10 11 events S/B 2  1.7 pt > 1 GeV/c 200k events ~ 8 sec Shown: central (b=0fm) Au+Au collisions at 25 AGeV Mass resolution: 13.6 MeV (  ) and 44 MeV (J/  ) LMVM spectra for SIS100 show similar quality J/  in central pAu at 30GeV with S/B=1.25 („thick“ 1% int. length target) J/    

20 Claudia Höhne Quark Matter, Darmstadt, May 2014 Cocktail/ Background distribution for LMVM 20 For both setups Cocktail/Background ratios of about 100 are reached in central Au+Au collisions at 25 AGeV for m inv ~ 0.5 – 0.6 GeV/c 2 Cocktail/Background muons electrons

21 Claudia Höhne Quark Matter, Darmstadt, May 2014 Acceptance –  -meson 21 muons Central (b=0fm) Au+Au collisions at 25 AGeV Midrapidity at 2 electrons

22 Claudia Höhne Quark Matter, Darmstadt, May 201422 RICH radiator box filled with CO 2 elaborated gas system test with mixed e-  beam from 2-10 GeV/c RICH Detector real dimension prototype in test beam at CERN, October 2011, 2012 approved Related Posters RICH detector development: M-09, M-10, M-11 momentum scan e  typical single event display! ≥ 20 hits/ ring noise/channel ~10Hz

23 Claudia Höhne Quark Matter, Darmstadt, May 201423 TRD detector beamtest at CERN, October 2011, 2012: 2011: test 12 different chamber types (w & w/o drift, distances…) test different radiator types (fibers, foils, foams) very nice agreement of simulated and measured data for the energy spectra 2012: real dimension chambers succesfully tested (59x59)cm 2 e-spectrum In preparation

24 Claudia Höhne Quark Matter, Darmstadt, May 2014 MUCH detector 24 Several succesful testbeam campaigns at CERN and COSY including a „mini-MUCH“ setup with absorbers > 90% efficiency, rate capability ok Large triple GEM chamber built (31x31 cm 2 ), sector based readout submitted Related Poster MUCH detector development: M-03

25 Claudia Höhne Quark Matter, Darmstadt, May 2014 Summary 25 FAIR construction progressing well: first beams 2018 CBM  Status of experiment preparation: Prototype detector performances fulfill CBM requirements, TDRs!  Funding: Substantial part of the CBM start version for SIS100 is financed (incl. planned applications) Di-Lepton feasibility studies in CBM:  Di-Muons: simulations based on realistic assumptions on signal cocktail, background and detector responses; next step: Implementation of straw-tube detectors for the stations 4 and 5  Di-Electrons: detailed investigation of background performed; next step: realistic detector description (TRD, TOF), further optimization (MVD)  Photons (not shown): Proof of principle ok, more details soon  All measurements well feasible with very good S/B ratios; di-electrons and di-muons complementary for detailed investigation of baryon dominated matter

26 Claudia Höhne Dense Baryonic Matter in the Cosmos and the Laboratory, Tübingen 2012 26 CBM collaboration Russia: IHEP Protvino INR Moscow ITEP Moscow KRI, St. Petersburg China: Tsinghua Univ., Beijing CCNU Wuhan USTC Hefei Croatia: University of Split Romania: NIPNE Bucharest Bucharest University Poland: Krakow Univ. Warsaw Univ. Warsaw Univ. of Tech. Silesia Univ. Katowice Nucl. Phys. Inst. Krakow Ukraine: KINR, Kiev Shevchenko Univ., Kiev FIAS Frankfurt Univ. Münster FZ Rossendorf GSI Darmstadt FAIR Darmstadt Univ. Tübingen Univ. Wuppertal Czech Republic: CAS, Rez Techn. Univ. Prague Germany: TU Darmstadt Univ. Gießen Univ. Heidelberg, Phys. Inst. Univ. Heidelberg, ZITI Univ. Frankfurt Hungaria: Wigner IPNP, Budapest Eötvös Univ. Budapest India: Aligarh Muslim Univ., Aligarh IOP Bhubaneswar Panjab Univ., Chandigarh Gauhati Univ., Guwahati Univ. Rajasthan, Jaipur Univ. Jammu, Jammu IIT Kharagpur SAHA Kolkata Univ Calcutta, Kolkata VECC Kolkata Univ. Kashmir, Srinagar Banaras Hindu Univ., Varanasi Inst. of Tech., Indore, India Kurchatov Inst. Moscow VBLHEP, JINR Dubna 56 institutions, > 400 members GSI, April 2014 LIT, JINR Dubna MEPHI Moscow Obninsk State Univ. PNPI Gatchina SINP, Moscow State Univ. St. Petersburg Polytec. U. Korea: Pusan National Univ. France: IPHC Strasbourg

27 Claudia Höhne Quark Matter, Darmstadt, May 2014 Backup 27

28 Claudia Höhne Quark Matter, Darmstadt, May 201428 STS tracking – heart of CBM Challenge: high track density:  600 charged particles in  25 o @ 10MHz Task track reconstruction: 0.1 GeV/c < p  10-12 GeV/c  p/p ~ 1% (p=1 GeV/c) primary and secondary vertex reconstruction (resolution  50  m) V 0 track pattern recognition → make use of excellent tracking for background suppression and momentum determination for dileptons c  = 312  m radiation hard and fast silicon detector self triggered FEE high speed DAQ and trigger online track reconstruction 1m1m

29 Claudia Höhne Quark Matter, Darmstadt, May 2014 MUCH – tracking performance 29 Tracking performance for  from  and J/  embedded in central Au+Au events (UrQMD) at 25 AGeV of 77% and 95% respectively LMVM setup (reduced absorber length) J/  setup (full absorber length)

30 Claudia Höhne Quark Matter, Darmstadt, May 201430 Electron identification global tracking + matching efficiency (STS, RICH, TRD, TOF) ~ 68% for p = 2 GeV/c e-ID in all detectors required: RICH, TRD, TOF integrated numbers in brackets are for full momentum range Central Au+Au, 25 AGeV

31 Claudia Höhne Quark Matter, Darmstadt, May 2014 Invariant mass spectra - electrons 31 1.6 10 11 events 6.5% eff. S/B 2  1.7 pt > 1 GeV/c 200k events ~ 8 sec   =4.4%   =5.5%   =7.1% Shown: central (b=0fm) Au+Au collisions at 25 AGeV Mass resolution: 13.6 MeV (  ) and 44 MeV (J/  ) LMVM spectra for SIS100 show similar quality SIS100: J/  in central pAu at 30GeV

32 Claudia Höhne Quark Matter, Darmstadt, May 2014 Invariant mass spectra – muons 32 Shown: central (b=0fm) Au+Au collisions at 25 AGeV Mass resolution: 12 MeV (  ) and 29 MeV (J/  ) only due to momentum determination in STS LMVM spectra for SIS100 show similar quality J/  in central pAu at 30GeV with superb S/B ratio ε ρ = 0.66 % ε ω = 0.68 % ε η = 0.41 % ε φ = 1.04 % ε J/ψ = 5 % S/B 2  = 1.68

33 Claudia Höhne Quark Matter, Darmstadt, May 2014 SIS 100 – muons 33 Central Au+Au, 8AGeVpAu, 30 GeV

34 Claudia Höhne Quark Matter, Darmstadt, May 2014 SIS 100 – electrons 34 Central Au+Au, 8AGeVpAu, 30 GeV

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