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GSI Helmholtzzentrum für Schwerionenforschung GmbH Status of the FAIR Antiproton Target K. Knie
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GSI Helmholtzzentrum für Schwerionenforschung GmbH FAIR / CERN / FNAL pbar Sources FAIRCERN (AC+AA)FNAL E(p), E(pbar)29 GeV, 3 GeV25 GeV, 2.7 GeV120 GeV, 8 GeV acceptance 240 mm mrad200 mm mrad 30 mm mrad protons / pulse2 × 10 13 1 - 2 × 10 13 ≥ 5 × 10 12 pulse lengthsingle bunch (50 ns)5 bunches in 400 nssingle bunch 1.6 µs cycle time10 s4.8 s1.5 s
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar target / separator 29 GeV p target & collector pbar separator 240 mm mrad p = 3.82 GeV/c p/p = ±3%
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Main Components
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Target R.P. Duperray et al., Phys. Rev. D 68, 094017 (2003) seprator acceptance: p pbar = 3.82 GeV/c ± 3% From ~ 2.5 × 10 -4 pbar / (p cm target) ~ 5 × 10 -6 (or 2 %) are "collectable" z / cm y / cm E p = 29 GeV magnetic horn with 400 kA: θ ≤ 80 mrad Ni rod, 110 mm, d = 3 mm graphite air-cooled AL block
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Magnetic horn LTspice Simulation: Pulsed Horn Current power pulser room soil shielding duct with 60 cables stripline
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar target station
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Magnets in pbar separator CR type magnets (simplified chambers possible) CR-type yokes, rad. hard coils with polyimide insulation Q1-Q2 and Q3-Q4 will be combined to one longer magnet, respectively Special dipole radiation hard coil (100 MGy) upper part of yoke divided in pieces < 10 t (needed for exchange of the coil) high radiation, no vacuum
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GSI Helmholtzzentrum für Schwerionenforschung GmbH horizontal cut vertical cut Dose rates during operation (FLUKA): Construction permit
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar building target dump
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Residual dose rates / handling: Operation permit: (in work, positive responses from authorities for target exchange/disposal concept obtained)
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Residual dose rate around target station air BEAM concrete Handling Area iron
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Top view, beam from left to right. Inner part of target station is always shielded Transport concept in building 6c
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Transport concept in building 6c Transport container moves to the shaft (1-2). Crane of carrying frame of the shielding flask lifts up the component (3). Concept accepted in construction permit
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Detailed study from Kraftanlagen Heidelberg Presented already to authorities: Very positive response obtained Trolley Coupling system Rail system Front door (for intervention only) Inner door Transport concept in building 6c
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GSI Helmholtzzentrum für Schwerionenforschung GmbH 1 2 3 Transport concept in building 6c
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar shielding flask: technical design weight: 25 tons
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Conversion rates
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Production Cross Section Semiempirical formula: R.P. Duperray et al., Phys. Rev. D 68, 094017 (2003) Fit of experimental data available in 2003. Monte Carlo Codes used in addition: FLUKA, MARS
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Production Cross Section p = 3.82 GeV / c, E = 3 GeV, Bρ = 13 Tm
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Collectible pbars p pbar = 3.82 GeV/c ± 3% From ~ 2.5 × 10 -4 pbar / (p cm target) ~ 5 × 10 -6 (or 2 %) are "collectible" z / cm y / cm E p = 29 GeV Emax SIS 100 acceptance separator/CR CR max. 13 Tm magnetic horn 0 < p pbar < 80 mrad
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Collectible pbars
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Collectible pbars: Self Absorption Cu: pbar = 0.8 b p pbar
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Collectible pbars: MARS/FLUKA Cu: pbar = 0.8 b p pbar
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Collectible pbars: MARS Cu: pbar = 0.8 b p pbar
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Cu: pbar = 8.8 b p pbar C: pbar = 0.42 b Collectible pbars: Graphite Surrounding
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar Yield: Collection efficiency of the magnetic horn yield = pbars in the ellipse primary protons
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar Yield: Cu vs Ir (8.92 vs 22.65 g/cm³)
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GSI Helmholtzzentrum für Schwerionenforschung GmbH pbar Yield: Comparison to CERN Data To injection orbit of collector ring: pbar/p = 2×10 -5 × 0.85 × 0.7 = 1.2×10 -5 Exp. data from CERN (Baird 1998) to injection orbit: pbar/p = 0.45×10 -5 × 1.5 = 0.7×10 -5 scattering losses in air / aluminum losses in separator / during injection correction for different energies and emmitances
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GSI Helmholtzzentrum für Schwerionenforschung GmbH Summary For 1 antiproton in the CR 10 5 primary protons on the target are needed. I do not see room for significant improvements. All optimization steps* I can imagine are in the order of <20 %. * including a Li-lens instead of a horn
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