HADES Upgrade for DIRAC-Phase-1 P. Salabura Jagiellonian University Kraków, GSI Darmstadt.

Slides:



Advertisements
Similar presentations
The Physics of Dense Nuclear Matter
Advertisements

1 Pion beam tracker for HADES Jerzy Pietraszko CBM Collaboration Meeting, March 9-13, 2009, GSI, Darmstadt.
KVI test experiment with existing RPC types for NeuLAND.
Hadron Physics (I3HP) activities Hadron Physics (I3HP) is part of Integrated Activity of 6’th European Framework. Contract has a form of consortium of.
The physics of dense baryonic matter investigated with HADES Winter Workshop on Nuclear Dynamics February, 6 – 11, 2011 Winter Park, Colorado Joachim Stroth,
Dielectrons from HADES to CBM Bratislava (SAS, PI), Catania (INFN - LNS), Cracow (Univ.), Darmstadt,(GSI), Dresden (FZR), Dubna (JINR), Frankfurt (Univ.),Giessen.
Cold Nuclear Matter Effects on Open Heavy Flavor at RHIC J. Matthew Durham for the PHENIX Collaboration Stony Brook University
October-November 2003China - ALICE meeting1 PHOS in ALICE A PHOton Spectrometer with unique capabilities for the detection/identification of photons and.
The Physics Potential of the PHENIX VTX and FVTX Detectors Eric J. Mannel WWND 13-Apr-2012.
LV boards Detector 8 m 2 6 sectors 8 m 2 6 sectors 8 m 2 6 sectors EPICS CLIENT SCS for custom hardware is also based on EPICS, with the particularity.
Christian Müntz (Univ. Frankfurt) for the HADES Collaboration, CPOD Challenges in Physics & Instrumentation Results from Heavy Ion and Elementary.
RICH PylosR. Gernhäuser (TU-München) The HADES RICH High Acceptance Di-Electron Spectrometer The HADES Spectrometer Special requirements RICH setup.
Di-electron mass spectrum in 2 AGeV 12 C+ 12 C measured with HADES Romain Holzmann, GSI Darmstadt for the HADES collaboration  Introduction  the case.
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.
1 High Acceptance Di-Electron Spectrometer The activity of JINR for HADES project is performed in frame of theme /2005 with a first priority.
Dielectron production in C+C collisions at 2AGeV with HADES Jochen Markert For the HADES Collaboration.
D ATA ANALYSIS FROM THE CERN TEST EXPERIMENT ABOUT THE HADES ELECTROMAGNETIC CALORIMETER By : Tazio Torrieri Supervisor : Vladimir Wagner.
The Experimental Quest for In-Medium Effects Romain Holzmann GSI Helmholtzzentrum für Schwerionenphysik, Darmstadt at 23 rd Indian-Summer School of Physics.
Study of hadron properties in cold nuclear matter with HADES Pavel Tlustý, Nuclear Physics Institute, Řež, Czech Republic for the HADES Collaboration ,
PARTICLE IDENTIFICATION IN THE HADES SPECTROMETER AND PARTICLE PRODUCTION IN C+C AT 2 A GeV The HADES spectrometer installed at GSI Darmstadt is devoted.
“DIRAC-PHASE-1” – Construction stage 1 at the international Facility for Antiproton and Ion Research (FAIR) at GSI, Darmstadt Task 8 - HADES1 Resistive.
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.
NA57 D. Elia, INFN Bari (Italy)QM2004, Oakland - January 11-17, Energy dependence of K 0 and hyperon production at CERN SPS Domenico Elia INFN -
Di-electron measurements with HADES at SIS100 Motivation Motivation HADES di-electron results (SIS 18) - summary HADES di-electron results (SIS 18) - summary.
ICPAGQP 2005, Kolkata Probing dense baryonic matter with time-like photons Dilepton spectroscopy from 1 to 40 AGeV at GSI and FAIR Joachim Stroth Univ.
Motivations - HADES Dielectron analysis strategy Results & models comparison C+C 2 AGeV C+C 1AGeV HADES experiment: dilepton spectroscopy in C+C (1 and.
Victor Ryabov (PNPI) for the PHENIX Collaboration QM2005 Budapest Aug,06, First measurement of the  - meson production with PHENIX experiment at.
A Silicon vertex tracker prototype for CBM Material for the FP6 Design application.
1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.
Experimental data by HADES PID method As an example let`s take deuterons and protons with p = 750 MeV/c. Their PDFs are gaussians with mean at β = p/(
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.
Mitglied der Leibniz-Gemeinschaft Institut für Kern- und Hadronenphysik HADES: High Acceptance Di-Electron Spectrometer at.
WWND 2011 Michael Weber for the HADES collaboration Inclusive e + e - pair production in p+p and p+Nb collisions at E = 3.5 GeV Introduction.
Upgrade of HADES and Electromagnetic Calorimeter CENAP board, January 15, 2010 P. Tlustý NPI Řež group, Czech Republic for the HADES Collaboration HADES.
RPC upgrade for the HADES Tracking: MDC e -,e + identification with RICH- TOF/PreShower  0.4 GeV/c TOF is not sufficient- Pre-Shower p,  identification.
Hadronic interaction studies with the ARGO-YBJ experiment (5,800 m 2 ) 10 Pads (56 x 62 cm 2 ) for each RPC 8 Strips (6.5 x 62 cm 2 ) for each Pad ( 
First experiments after HADES upgrade CENAP board, September 24, 2010 P. Filip, A. Kugler, O. Svoboda, Y. Sobolev, P. Tlustý, V. Wagner NPI Řež group,
Hadron production in C+C at 1 and 2 A GeV analysis of data from experiments NOV02 and AUG04 for high resolution tracking (Runge-Kutta tracks) Pavel Tlustý,
Status Report of DIRAC SPS and PS experiments Committee L. Nemenov 22 April 2008 DIRAC Addendum LIFETIME MEASUREMENT OF AND ATOMS TO TEST LOW-ENERGY QCD.
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.
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.
Hadron production in C+C at 1 and 2 A GeV analysis of data from experiments NOV02 and AUG04 for high resolution tracking (Runge-Kutta tracks) Pavel Tlustý,
Hadron production in C+C at 2 A GeV measured by the HADES spectrometer Nov02 gen3 analysis and results for spline tracks (shown in Dubna) changes - removing.
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.
Daniel Belver IX Workshop on RPC and Related Detectors, Mumbai February 13-16th 2008 Performances of the Front End Electronics for the HADES RPC wall in.
NSS2006Shengli Huang1 The Time of Flight Detector Upgrade at PHENIX Shengli Huang PHENIX Collaboration Outlines: 1.Physics motivations 2.Multi-gap Resistive.
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Future Experiments with HADES at FAIR Pavel Tlustý, NPI Řež “near future” - experiments on SIS18 in ? - upgrade of the HADES spectrometer experiments.
The Slow Control System of the HADES RPC Wall Alejandro Gil on behalf of the HADES RPC group IFIC (Centro Mixto UV-CSIC) Valencia, 46071, Spain IEEE-RT2009.
Dilepton production in p+p collisions at 3.5 GeV experimental results and their interpretation Anar Rustamov for the HADES collaboration GSI Helmholtzzentrum.
The HADES timing RPC Inner TOF Wall P.Fonte for the HADES RPC group DIRAC phase1 9th International Workshop on Resistive Plate Chambers and Related Detectors.
1 More information: Status Report of HADES Project (JINR Participation) Theme: /2005 Leaders:
Beam detectors in Au+Au run and future developments - Results of Aug 2012 Au+Au test – radiation damage - scCVD diamond detector with strip metalization.
for the HADES Collaboration
Dielectron Spectroscopy
eTOF - status and plan CBM-STAR joint Workshop Outline Introduction
Performance of the HADES-TOF RPC wall in a Au-Au beam
Beam detectors performance during the Au+Au runs in HADES
RPC with strip readout Last results from test of timing glass
Performance of timing-RPC prototypes with relativistic heavy ions
Highlights from HADES Au+Au collisions at 1.23 AGeV
Tracking results from Au+Au test Beam
Simulation results for the upgraded RICH detector in the HADES experiment. Semen Lebedev1,3, Jürgen Friese2, Claudia Höhne1, Tobias Kunz2, Jochen Markert4.
Participation in the HADES experiment
Recent results from exclusive ppppe+e- reactions with HADES
New Strangeness Results from HADES
Jerzy Pietraszko, HADES at SIS100 - status GSI Darmstadt, Germany
Presentation transcript:

HADES Upgrade for DIRAC-Phase-1 P. Salabura Jagiellonian University Kraków, GSI Darmstadt

HADES GSI 20 institutions from 20 countries 1994 approved 2002 first production run

Physics runs conducted November 2002: C+C 2 AGeV, commissioning and physics runs 220 Mevents – two level trigger scheme (LVL1/LVL2)220 Mevents – full coverage with inner MDCI/II, 2 sectors complete tracking (MDCI-IV)  inclusive e+,e- production ("DLS enhancement") February 2004: p+p 2.2 GeV 400 Mevents –LH 2 target400 Mevents –complete tracking in 4 sectors, 2 sectors with MDC(I-III)  exclusive meson reconstruction August 2004: C+C 1AGeV –complete tracking in 4 sectors, 2 sectors with MDC(I-III) 650 Mevents  inclusive e+,e- production ("DLS enhancement" 650 Mevents 2200 Mevents September 2005: Ar+KCl 1.75 AGeV 2200 Mevents –complete tracking in 4 sectors, 2 sectors with MDC(I-III)  inclusive e+,e- production: vector mesons in medium

 M/M(  )= 10%. no outer tracking within acceptance 16k signal S/B>1 for M>140 MeV/c 2 Corrected for Reconstruction Efficiency Inside HADES geometrical acceptance, no extrapolation to 4  ! Compared with a cocktail based on known or m t -scaled meson multiplicities and their vacuum decay properties. Dielectrons from 2 AGeV

Exclusive meson reconstruction in 2.2 GeV pp→pp  →pp  +  -  0 pp→pp  →ppe + e -  00  Hadronic channels Electromagnetic channels pp→pp  0 →ppe+e-   =14 MeV/c 2 (pp  /e +  /e - ) missing mass vs (pp) missing mass distributions

future upgrades Needed for : (I) HI systems with at 1-2 AGeV A tot >80 (II) FAIR (8AGeV) (III) High intenisty pion beams RPC ( inner time-of-flight) → essential for HI, important for elementary channels with strangeness production (  /K separation) (FP6 construction -> P. Fonte) Forward hodoscope → essential for p+d, important for HI (FP6 construction-> H. Stroebele) Pion tracking → essential for  +p,  +HI DAQ → essential for HI (FP6 construction-> M. Traxler)

HADES1-TOFINO replacement by RPC TOFINO:(time-of-flight between o) –4 paddles per sector only –limited resolution (450 ps) –insufficient granularity for HI TOFINO target RPC: 180 cells/sector (double hit<10% for 1.0 AGeV Au+Au) time resolution < 100 ps Granularity: 1080 cells

operational parameter matched to HADES overall performance granularity: double-hit probability below 10% resolution: 100 ps (s) or better rate capability: up to 600 Hz/cm2 (at forward) efficiency: above 95% for single hits concept of the design: shielded single cells 4 gaps with commercial glass 2mm thick common gas box sector-wise customized read-out: FEE (preamp, discriminator, TimeOverThreshold) + TDC (128 channels) based on HPTDC & CPU with fast ethernet RPC for HADES Gas mixture: 98.5% C 2 H 2 F 4 + 1% SF % i-C 4 H 10 Potential = 3 kV All full-size components produced and tested 30 months duration workplane details in talk of P. Fonte

HADES2-Forward hodoscope Collective observables for dilectron production in HI collisions (flow) event plane determination measurement of reaction centrality Spactator tagging for d+p reactions direct comparison of dielectron production in pp and p+n reactions Upgrade of old and well known KAOS FH: inspection of detectors (380 modules), new reflecting cover for light guides, mainframe modifications new digital (TDC) electronic – same as used for the RPC new HV and slow control system Total project duration 12 months → see talk of H. Stroebele for workplan details Acceptance for charge particles with  < 8 0

HADES3 – DAQ upgrade (1) Exchange of CPUs for event building for more efficient transport of large events. x86 CPUs running under LINUX and featuring GIGAbit Ethernet successfully tested in the last Ar+KCl beam time (2) New Image Processing Unit for Time of Flight and RPC detector essential for heavy systems (A tot >80) with large multiplicities (3) New Matching Unit for faster processing of second level trigger in large multiplicity environment essential for heavy systems (A tot >80 ) with large multiplicities Final goal is to reach 20 KHz LVL1 trigger rate (presently 7kHz) Total duration 26 months → see talk of M. Traxler for workplan details

time line  on p, A p, on p, d AA collisions DIRAC

Allocated man power and investment 5 institutions: GSI Darmstadt, Institute fuer Kernphysik Frankfurt (IKF), Jagiellonian University (JU) Kraków, University Santiago de Compostella (USC), Laboratório de Instrumentação e Física Experimental de Partículas (LIP) Coimbra, Nuclear Physics Institute (INR) Rez, Institute for Nuclear Reasearch Moscow 3 tasks: HADES1- RPC (P.Fonte), HADES2-FH (H.Stroebele), HADES3-DAQ (M. Traxler) Man power : DIRAC Investment (k€): DIRAC All Total

HADES collaboration 1)Institute of Physics, Slovak Academy of Sciences, Bratislava, Slovakia 2)Istituto Nazionale di Fisica Nucleare - Laboratori Nazionali del Sud, Catania, Italy 3)Dipartimento di Fisica e Astronomia, Università di Catania, 95125, Catania, Italy 4)LIP-Laboratório de Instrumentação e Física Experimental de Partículas, Departamento de Física da Universidade de Coimbra, Coimbra, Portugal 5)Smoluchowski Institute of Physics, Jagiellonian University of Cracow, Cracow, Poland 6)Gesellschaft für Schwerionenforschung mbH, Darmstadt, Germany 7)Joint Institute of Nuclear Research, Dubna, Russia 8)Institut für Kernphysik, Johann Wolfgang Goethe-Universität, Frankfurt, Germany 9)II.Physikalisches Institut, Justus Liebig Universität Giessen, Giessen, Germany 10)Istituto Nazionale di Fisica Nucleare, Sezione di Milano, Milano, Italy 11)Dipartimento di Fisica, Università di Milano, Milano, Italy 12)Institute for Nuclear Research, Russian Academy of Science, Moscow, Russia 13)Institute of Theoretical and Experimental Physics, Moscow, Russia 14)Physik Department E12, Technische Universität München, Garching, Germany 15)Department of Physics, University of Cyprus, 1678 Nicosia, Cyprus 16)Institut de Physique Nucléaire d'Orsay, CNRS/IN2P3, Orsay, France 17)Nuclear Physics Institute, Academy of Sciences of Czech Republic, Rez, Czech Republic 18)Institut für Kern- und Hadronenphysik, Forschungszentrum Rossendorf, PF , Dresden, Germany 19)Departamento de Física de Partículas. University of Santiago de Compostela Santiago de Compostela, Spain 20)Instituto de Física Corpuscular, Universidad de Valencia-CSIC,46971-Valencia, Spain

Comparison with transport theory RQMD calculation: D. Cozma, C. Fuchs and A. Faessler, Tübingen Filtered with HADES acceptance resolution smeared vacuum calculation in-medium calculation collisional broadening extended VDM + decoherence Brown-Rho scaling of VMs  See Phys. Rev. C68 (2003) for details.