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The HADES experiment @GSI
Collaboration: 18 Inst members Motivation Detector description Performance outlook
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Motivation Dalitz and two-body decays, pN, N reactions
Properties of hadrons in strong int. matter: M, G vs r, mB, T, V Vector meson , , spectral functions measurements Hadron’s structure: VDM, Form factors, vector meson-nucleon inter. Dalitz and two-body decays, pN, N reactions SIS / GSI : heavy ion, proton,pion beams 0 r 3 r T 80 MeV HADES: systematic dielpton spectroscopy meson prod. in pp / pp : r = 0 , T = 0 MeV meson prod. in pA / pA : r = r0 , T = 0 MeV meson prod. in AA : r = 1-3r0 , T = 80 MeV
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High Acceptance DiElectron Spectrometer
Magnet SC. toroid ( 6 coils) 2p in f o < J < 85o Lepton Identification RICH C4F gas Phot. Det CsI - cathode META TOF scintillator wall + Pre-Shower detector p/ identification META and tracking Tracking p – measurement, vertex reconstruction MDC Drift chambers dx ~ 80 mm (s)
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PreShower Magnet Coils RICH RICH +MDC I Back view
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HADES S.C. Magnet ILSE SC Toroid Beam operation Imax = 3465 A
Bmax = T Bmax = T Dp (q=25°) = 103 MeV/c Dp (q=80°) = 60 MeV/c Beam operation I = 2500 A Dp (25°) = 74 MeV/c coil air
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Ring Imaging CHerenkov Detector
e+e- - identification Cherenkov light cos qc= 1/ ß.n(l) N = N0. lrad .1/ gt ( lrad = 40 cm ) N0 det. characteristics Radiator (hadron blind!) 3 ~ ghad < gt < glep C4F10 : gt = 18.3 pp> 3 GeV/c VUV - Mirror Poly-C substr. (2 mm) x/X < 2% Al + MgF2 coating R > 80% Photon detector (MWPC) CsI - cath. CaF2 window
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RICH in parts Photon detector with CaF2 window & CFK radiator shell
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RICH rings g e+ p0 Q ~ 2.20 e- g Q ~ 0.70 Strong sources lead to large
Dalitz Strong sources lead to large comb. backgr.!!! g e+ e- Q ~ 0.70 Conversion
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Multiwire Drift Chambers
0.7 % mass resolution in the r/w - region Combinatorial background reduction – e+,e- close pair rejection
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Multiwire Drift Chambers
IPN Orsay FZR LHE Dubna GSI 4 layer/sector. total 33 m3 active area, cells y<100 m plane resolution He-iC4H10 [60-40] gas mixture and low Z material GSI plane ORSAY plane MDC: participating Institutions: I: GSI, II: LHE/JINR Dubna, III: FZ Rossendorf, IV: IPN Orsay
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MDC module x/X0 Cell characteristic 6 [mm]
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Performance of MDC Intrinsic spatial resolution:
Proton beam, silicon tracker “In-beam” (C+C 1.8 AGeV) Layer efficiency: > 98% Orsay FZR Dubna GSI Chamber Number Spatial Resolution (microns)
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MDC Read-out Daughterboards ASD8 LVL1-connector FPC- connector TDC
Motherboard Analog Read-out: Differential amplifier, ASD8 chip, 8 channels, 1 fC intr. Noise, 30 mW/channel adjustable threshold (one for 16 channels) TDC Features: (8 channels per chip) 8 channels per chip 250/500 ps/channel “2 times (t1, t2) – multi-hit capable Zero & spike (t1-t2 < 20ns) suppression Calibration Mode (…mixed trigger “Time above threshold” (…signal shape, charge): Efficient Offline noise suppression!
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TOF >450 dt : 90 – 140 ps Ch. p. distribution for C+C @ 1.5 AGeV
Outer TOF wall >450: 6 * 64 scint. Installed. T line fully operational dt : 90 – 140 ps dE/dx measurement tracking J. Friese, TU München
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TOF-hadron identification
Preliminary p [MeV/c] b Mass [MeV/c2] counts Tof [ns] Energy loss [MeV] Mass [MeV/c2] counts Deuteron peak: m0 = 1890 MeV sm = 551 MeV deuterons protons
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TOF-RICH lepton identification
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Pre-Shower/TOF system <450
Pre-conv Post1-conv Post2-conv. esingle80% Pads TOFINO tof measurement t0.35 ns Field Sense wires 2 radiation lengths Pb converter target Pre-Shower detector side view beam 3 pad chambers (20000 pads) em. showers in Pb converters
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C+C 1.5 AGeV p beam e- beam Shower candidate
One event: detector response Pre-converter Post1-converter Post2-Converter p beam e- beam Shower candidate Pre-Conv Pre-Conv Post1-Conv Post1-Conv
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RICH-MDC-META lepton identification
Data: Nov01 C-C 2.0 AGeV magnetic field preliminary q* momentum Log z! tof [ns] tof [ns] q*momentum
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RICH-MDC-META lepton identification
Data: Nov01 C-C 2.0 AGeV magnetic field preliminary Full HADES simulation and data analysis RQMD ev.generator simul. Ne/N+ RICH-Track(MDC-META) RICH & fast tof &shower MDC I/II (inner ) e- e+ q* momentum [e*MeV/c]
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HADES Trigger System Needs level 2 trigger: 107- 108 paricles/s
Ring recognition in RICH Hit finding and tof calculation in TOF El. Shower search in Pre-Shower RICH and META candidate matching via azimuthal correlations Selection of e+e--pairs (momentum and invariant mass analysis) High rates (105 Hz) 10ms max. LVL2 trigger decision time) Parallel- und Pipeline architecture FPGAs, CPLDs and DSPs paricles/s 105-6 interactions/s (1% target) Level 1 Trigger: Multiplicity in TOF 104 _105 central events/s Large data rate 3 GByte/s
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Second Level trigger flow
dilepton 1:100
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Trigger distribution system
Trigger distribution: LVL1 (TOF Mult.) and LVL2 (MU) via CTU DAQ synchronized via event number distribution Total: 50 VME-Modules
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RICH IPU 1 ring search mask (13x13 pads)
Pattern reconstruction (96x96 pad plane) Ring recognition fixed 80 pads mask ( ring/ veto region) local maximum search IPU-algorithm X correlation Hits found by the IPU and not by the algorithm Hits found by the algorithm and not by the IPU 0.2% X ALGO (pads) X IPU (pads) uncorrelated emulation rings X (pads) Y (pads) Data: Nov01 C-C 1.5 AGeV full field Discrepancy: 0.4%
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Matching Unit Preliminary lepton
Data: Nov01 C-C 1.5 AGeV magnetic field Reference System: offline analysis leptons LVL2 conditions in the MU: 1 hit in RICH 1 hit in TOF Df < 15° lepton Trigger condition % evts evt >= 1 ring 10.5% evt >= 1 lepton 2.9% evt >= 2 rings 4.6% evt >= 2 leptons 1.7% evt >= 1 dilepton 0.3% Efficiency RICH IPU LVL2 integrated eff 85.3% 84.7% event eff 87.3% 86.6% N. fakes ele/evt
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Outlook HADES comes into operation(e/p/p sep., LVL2 trig., tracking)
3 MDC layer will be completed this summer (p3% for /) DAQ and LVL2 trigger commisioning Phase I (2002 – 2003) : (acc. proposals S200 ,S262) Continuum below M inv < 600 MeV/c2 ; 0 Dalitz in C+C High statistics e+,e- production in HI reactions C+ C @ 1 – 2 AGeV (compare to DLS) e+e- production in p- p p- p @ 0.8 – 1.3 GeV/c (below and above threshold for r/w e+e- pair acceptances pp pp h pp e+e-
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e+e- pairs in C + C collisions
Ebeam = 1A GeV/c Simulation for 3 MDC setup : needs 2 * 109 events ~ 5 days 89000 e+e- Ebeam = 2A GeV/c
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e+e- pairs in -+p reactions
Pbeam = 0.8 GeV/c Simulation for 3 MDC setup : 7 days of p- beam @ 1 * 106 s-1 !! Pbeam = 1.3 GeV/c
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Collaboration Bratislava (SAS, PI) Catania (INFN - LNS)
Clermont-Ferrand (Univ.) Cracow (Univ.) Darmstadt (GSI) Dresden (FZR) Dubna (JINR) Frankfurt (Univ.) Giessen (Univ.) Milano (INFN, Univ.) Moscow (ITEP, MEPhI, RAS) Munich (Tech. Univ.) Nicosia (Univ.) Orsay (IPN) Rez (CAS, NPI) Sant. de Compostela (Univ.) Valencia (Univ.)
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