D DD*DD* ψ(1 1 D 2 ) ψ(1 3 D 2 ) ψ(1 3 D 3 ) ψ(1 3 D 1 ) η c (1 1 S 0 ) η c (2 1 S 0 ) J/ψ(1...

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DD DD* ψ(1 1 D 2 ) ψ(1 3 D 2 ) ψ(1 3 D 3 ) ψ(1 3 D 1 ) η c (1 1 S 0 ) η c (2 1 S 0 ) J/ψ(1 3 S 1 ) χ c0 (1 3 P 0 ) χ c1 (1 3 P 1 ) χ c2 (1 3 P 2 ) h 1c (1 1 P 1 ) D*D* ψ(3 3 S 1 ) ψ(2 3 S 1 ) χ c0 (2 3 P 0 ) χ c1 (2 3 P 1 ) χ c2 (2 3 P 2 ) h 1c (2 1 P 1 ) η c (3 1 S 0 ) Hadron Physics @ Klaus Peters KPIII/HPI, GSI Darmstadt IKF, JWGU Frankfurt Project X Workshop “Physics” Nov 16, 2007

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  • Hadron Physics @ Klaus PetersKPIII/HPI, GSI Darmstadt IKF, JWGU FrankfurtProject X Workshop PhysicsNov 16, 2007

    Klaus Peters - Hadronphysics @ FAIR

  • Nov. 7, FAIR Start-Event last week

    Offical Start SignedBy 12 Partners

    Volume in Phase A940 M

    16 Countries

    Klaus Peters - Hadronphysics @ FAIR

  • Where is Darmstadt ?GSI

    Klaus Peters - Hadronphysics @ FAIR

  • @ GSIFAIRCDR 2001FTBR 2006Construction Start 2007Ground Breaking 2008First Experiments 2012Fully Completed 2015Budget 1.1 BExisting GSInew FAIR buildings

    Klaus Peters - Hadronphysics @ FAIR

  • Structure of Mattergalaxy1021 mmatter10-1 mcrystal10-9 matom10-10 matomic nucleus10-14 m

  • Mission StatementStrong and weak interaction critically determine the structure of matter at the microscopic level

    Goal: Comprehensive and quantitative understanding

    Many-body aspects play an important role at all levels of the hierarchical structure of matter

    Goal: Investigate many-body effects at all scales

    Klaus Peters - Hadronphysics @ FAIR

  • Five Areas of Research at FAIR 100 mHadron Physicswith antiprotonsNuclear Structure & Astrophysicswith radioactive beams Plasma Physics with compressed ion beams & high-intensity petawatt-laserNuclear Matter Physics with35-45 GeV/u HI beamsHigh EM Field (HI)Fundamental Studies (HI & p)Applications (HI)

    Klaus Peters - Hadronphysics @ FAIR

  • Accelerator ChainSIS 100SIS 12/18SIS 300SIS 300High Energy operation SIS300Highly Parallel OperationSIS 300

    Klaus Peters - Hadronphysics @ FAIR

  • Phase diagram of strongly interacting matterSPS, RHIC, LHC:high temperature, low baryon densitySIS300:moderate temperature, high baryon density

    Klaus Peters - Hadronphysics @ FAIR

  • CBM Experiment - ObjectivesIn-medium modifications of hadrons onset of chiral symmetry restoration at high Bmeasure: , , e+e- and open charm (D mesons) Strangeness in matter (strange matter?)enhanced strangeness production ?measure: K, , , , Indications for deconfinement at high Banomalous charmonium suppression ?measure: J/, DCritical point event-by-event fluctuationsColor superconductivityprecursor effects ?

    Klaus Peters - Hadronphysics @ FAIR

  • CBM @ FAIRRadiation hard Silicon Tracking System(pixel/strip) in a magnetic dipole fieldElectron detectors: RICH & TRD & ECAL:pion suppression better 104Hadron identification: TOF-RPCMeasurement of photons, , , and muons: electromagnetic calorimeter (ECAL)High speed data acquisition and trigger system

    Klaus Peters - Hadronphysics @ FAIR

  • QCD phases @CBMCBM (Phase B)EOI 2000LOI 2004TPR 2005TDRs 2009 - 2010Construction2009 -2015 1st Physics2016Cost 60 M

    Klaus Peters - Hadronphysics @ FAIR

  • The Fluxtube in a Meson0.7 fm1.0 fm1.35 fmstrong interaction strengthLattice QCD calculations G. Bali, hep-lat/9409005[qq] bound state RotationVibration

    Klaus Peters - Hadronphysics @ FAIR

  • The Potential A GuideG. Bali et al., hep-lat/0003012G. Bali, hep-ph/0412158

    Klaus Peters - Hadronphysics @ FAIR

  • X(3872) and Confirmationhep-ex/04060229.411.6 BABARPhys. Rev. Lett. 91(2003)262001 152 Mill. BB

    Klaus Peters - Hadronphysics @ FAIR

  • Why Antiprotons for Heavy Flavour Spectroscopyhigh resolution spectroscopy with p-beams in formation experiments:E Ebeam e+e- interactions:Only 1-- states are formedOther states only by secondary decays moderate mass resolutionpp reactions:All states directly formedvery good mass resolutionCBall, Edwards et al. PRL 48 (1982) 70E835, Ambrogiani et al., PRD 62 (2000) 052002

    Klaus Peters - Hadronphysics @ FAIR

  • Why Antiprotons for Heavy Flavour Spectroscopyhigh resolution spectroscopy with p-beams in formation experiments:E Ebeam Precision Frontier

    high yield of gluonic and radial excitations in pp glueballs, charmed hybrids Discovery Potential

    event tagging by pair wise associated production,(particle, anti-particle) e.g. ppDD

    large s at low momentum transferimportant for in-medium "implantation" of hadrons:study of in-medium effects of charmed states

    Klaus Peters - Hadronphysics @ FAIR

  • Electromagnetic Reactionse-pe-pppppe+e-pp

    Klaus Peters - Hadronphysics @ FAIR

  • Crossed-Channel Compton ScatteringCross section 2.5pb @ s 10 GeV2L = 21032 cm-2 s-1 103 Events/MonthElectromagnetic Formfactor of the Proton (time-like)

    Klaus Peters - Hadronphysics @ FAIR

  • Accessible Charmed Hadrons at PANDAOther exotics with identical decay channels same regionconventionalcharmoniumexoticcharmonium

    Klaus Peters - Hadronphysics @ FAIR

  • HESR Storage Ring for AntiprotonsParameters of HESR Injection of p at 3.7 GeV Slow synchrotron (1.5-14.5 GeV/c) Storage ring for internal target operation Luminosity up to L~ 2x1032 cm-2s-1 Beam cooling (stochastic & electron)ECMResonance scan Energy resolution ~50 keV Tune ECM to probe resonance Get precise mass and width

    Klaus Peters - Hadronphysics @ FAIR

  • PANDAHigh luminosity modeLuminosity = 2 x 1032 cm-2s-1p/p ~ 10-4 (stochastic cooling)High resolution modep/p ~ few 10-5 (+electron cooling)Luminosity > 1031 cm-2s-1Gas-Jet/Pellet/Wire Targetpp

    Klaus Peters - Hadronphysics @ FAIR

  • p @HESRNESRPANDAFLAIRPANDA (Phase A)EOI 1999LOI 2004TPR 2005TDRs 2009 - 2010Construction2009 -2013 1st Physics2014Cost 57 M

    Klaus Peters - Hadronphysics @ FAIR

  • First cold Anti-Hydrogen 2002 @ ADATHENA Nature 419 (2002) 456ATRAPNested Penning trapscatch energy: some keVUltimate Resolution: neutral atom traps and laser cooling to milli-Kelvin temperatures - Long Term Project - FAIR

    Klaus Peters - Hadronphysics @ FAIR

  • FLAIR Physics Overview (Antiprotons)Spectroscopy as Test for CPT and QEDAntiprotonic atoms (p-He, p-p), anti-hydrogenGravitation of anti-matterTrapped and laser-cooled anti-hydrogenAtomic CollisionsIonization, energy loss, anti-matter-matterAntiprotons as hadronic ProbesX-rays of light p-Atoms: Low energy QCDX-rays of neutron rich nuclei: nuclear structure (halo)Antineutron interactionStrangeness 2 productionMedical application: Tumor therapyHigh-brilliantLow energy beams

    USR

    DC beam,rare ions

    Higher energies

    Klaus Peters - Hadronphysics @ FAIR

  • FLAIR Facility for Low-energy Antiproton and Ion ResearchNESRp & Ions 30 400 MeVLSR:Standard Ring < 300 keVUSRElectrostatic< 20 keVHITRAPp & Ions stopped & extracted @ 5 keV

    CRYRING

    Challenge! newMPI-K HD

    In construction for ESR @ GSIwith Hall Aof CDR

    Klaus Peters - Hadronphysics @ FAIR

  • Thank You

    Klaus Peters - Hadronphysics @ FAIR


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