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The CERN Antiproton Decelerator AD Status and Future

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Title: The CERN Antiproton Decelerator AD Status and Future


1
The CERN Antiproton Decelerator (AD)Status and
Future
  •  
  •  

2
Introduction
  •  
  •  
  • Based on a previous CERN machine (the Antiproton
    Collector AC), AD started producing low-energy
    antiproton beams for physics in 2000. Here we
    will discuss problems linked to ADs co-existance
    with CERN main programs and recent decisions
    taken with regard to ADs future.

3
Background
  • 1980-1986 AA
  • 3.57 GeV/c Antiproton Accumulator ring
  • 1012 pbars stored (peak). p/pbar collisions in
    SPS
  • 1986-1996 AAC (AAAC)
  • Large acceptance Antiproton Collector ring added.
    Production rate increased 10-fold to 61010
    pbars/h
  • low energy experiments in LEAR
  • 1998 - ? AD
  • AC converted from fixed energy storage ring to
    Decelerator. 5107 pbars slowed down to 100 MeV/c
    (5.3MeV kinetic). Local experimental area.
  • Fast extraction for Penning traps other low
    energy exp.
  • ATRAP Production and study of trapped Hbars
  • ALPHA Production and study of trapped Hbars
  • ASACUSA Spectroscopy on Antiprotonic helium,
    traps etc. etc.
  • ACE Biological effect of Pbars gt tumor
    treatment

4
(No Transcript)
5
AD
  • Basic Parameters
  • Circumference 182 m
  • Production beam 1.51013 protons/cycle
  • Injected beam 5107 pbars/cycle
  • Beam momenta max-min 3.57 0.1 GeV/c
  • Momenta for beam cooling
  • Stochastic 3.57 and 2.0 GeV/c
  • Electron 0.3 and 0.1 GeV/c
  • Transverse emittances h/v 200 1 p.mm.mrad
  • Momentum spread 610-2 110-4 dp/p
  • Vacuum pressure, average 410-10 Torr
  • Cycle length 100 s
  • Deceleration efficiency 85

6
Operation statistics
7
2009 run
  • Key dates
  • 23/4 Ring closure, start HW-tests
  • 11/5 Start setting up with beam
  • 8/6 start physics

8
AD Consolidation
  • Many HW breakdowns of major components since
    2004 several ring/transferline magnets, vacuum
    leaks, power supplies etc.
  • Lengthy repairs due to lack of spares, need for
    vacuum bakeout, obsolete equipment, loss of
    know-how etc.
  • Reduced AD maintenance/support due to other CERN
    priorities
  • gt
  • Limited consolidation budget for urgent measures
    granted following approval of AD running 2007 -
    2010
  • Consolidation budget requested in 2008 for
    continued AD operation in the medium/long term
  • Focus is mainly on consolidating existing
    equipment
  • The two scenarios under consideration are
  • (1) Continued operation until the end of 2012
    with no major modifications to the AD machine
  • (2) Operation until the end of 2016 with the
    possibility to implement the proposed ELENA
    upgrade.

9
AD Consolidation
  • Analysis of breakdown risks, identification of
    items and costs for consolidation was done as
    well as a risk score classification.
  • Some 40 items have been identified, costs
    (manpowermaterial) estimated and summed up for
    the 2 scenarios 2012/2016.
  • The matter was discussed at the Research Board
    meeting 5/12/09 It was decided to execute
    approx. 1/3 of the proposed 2016 consolidation
    program. Quote
  • Since AD operation will be incompatible with the
  • new PS2, this sets a clear end-point to the
    programme in 2017. It was agreed that the
  • strategy to be followed should have the aim of
    maintaining the AD facility
  • operational until then, but consistent with the
    budgetary constraints.

10
Proposed new experiment AEGIS
  • The proposed AEGIS experiment was in principle
    approved as AD-6 at the RB meeting 5/12/09.
    Budgetary details remain to be worked out.
  • Standard fast extraction of the 100 MeV/c beam
  • The extension of the existing ACE beamline has
    been foreseen since the beginning of AD and
    requires manufacturing and installation of 2
    quadrupoles, 1 dipole, 3 combined H/V corrector
    magnets and 3 bpms as well as vacuum chambers
    and equipment.
  • Work is planned to be started in 2009, first beam
    in 2011

11
Long-term AD future
  • AD and antiprotons. According to the planning of
    the FAIR project, the antiproton facility in GSI
    should have succeeded to the AD after the year
    2017. The continuation of antiproton experiments
    at CERN after the PS complex is decommissioned is
    therefore unlikely. In spite of this, if an
    antiproton facility is still needed on the CERN
    site, the following scenarios can be envisaged
  • For a limited period of time (1-2 years) the old
    PS complex could be kept active and dedicated to
    the production of antiprotons.
  • For continuation in the medium term, the AD
    target could receive a proton beam from PS2 via a
    1.3 km transfer line, using a new 650 m long
    tunnel and passing through 3/4 of the PS ring.
  • For continuation in the long term, a new and
    modern antiproton facility with its target area
    should be built in a cavern close to PS2.

12
Connection to AD for continued Pbar physics in
the medium term.
13
In the long term, a new antiproton facility could
be built either 40m underground or in a surface
building further away from PS2
Possible PS2 surface experimental area
Possible PS2 underground experimental areas
14
Sideview of baseline scheme
15
Long-term AD future
  • May 09 meeting to discuss Non-LHC physics
  • Objective is to define strategies for optimizing
    physics output at CERN and world-wide
  • We might know more about the future of low-energy
    pbar physics after that..

16
AD future improvements ELENA
17
ELENA basic parameters
18
AD future improvements ELENA
  • 3,5 years project duration
  • 10 MCHF 50 Man-years needed
  • CERN approval conditioned to external funding
    50/50
  • ELENA was not discussed during RB 5/12/09
  • External partners interested in participating in
    the project

19
TSR gt ELENA ?
  • A visit to the TSR facility at MPI-K Heidelberg
    has enabled us to verify the feasibility of using
    an appreciable amount of the TSR machine
    components for the construction of the proposed
    low energy antiproton ring, ELENA. Even thought
    the TSR ring size (53 m) does not fit the
    dimensions of the ELENA ring, which would have a
    circumference of about 30 m, most of the TSR
    elements could be used for the smaller ring.
  • Magnets All 8 bending magnets fit the
    requirements.
  • 20 quadrupole magnets are available, 8 are
    required for use in ELENA and the rest will be
    used in the transfer line or kept as spares.
  • Orbit correction The 8 backleg windings on the
    main bends will be used for the horizontal orbit
    correction. A total of 12 dipoles are available
    to correct the vertical orbit or to provide extra
    elements for the horizontal correction.
  • Injection ejection The magnetic and
    electrostatic septa of TSR could be adapted for
    use in ELENA. The kickers, however, do not fit
    the requirements. In addition an number of
    magnetic correctors can be used in the AD-ELENA
    transfer line.
  • Electron cooling It is proposed to use the
    electron target experiment as an electron cooler
    for ELENA. This device comes complete with the
    Faraday cage and high voltage platform. A
    modification to the electron gun will be needed
    in order to exchange the photocathode with a
    conventional thermionic cathode.

20
TSR gt ELENA ?
  • Vacuum All vacuum chambers are made of 316LN
    stainless steel and are bakeable. Turbo molecular
    pumps, ion pumps and Ti sublimation pumps can all
    be re-used in ELENA. In addition 5 sector valves
    are also available as well as vacuum gauges and
    residual gas analysers. Only the pumps and the
    valves are equipped with bakeout jackets. The
    rest of the machine is equipped with heating
    strips and insulating material. The complete
    control of the bakeout could also be used.
  • Instrumentation 8 horizontal/vertical pick-ups
    (LEAR type, fully bakeable) can be used to
    measure the closed orbit. The intensity is
    measured with a standard Bergoz BCT and the
    circulating beam profile is measured with
    ionization profile monitors and a scraper.
    Schottky pick-ups are installed but their use in
    ELENA might be limited due to the low number of
    particles. They would be useful for the tune
    measurement where a dedicated BTF kicker is
    available.
  • Taking the above into consideration, we estimate
    that between 2.5 to 3 MCHF could be saved by
    using TSR elements in the construction of the
    ELENA post-decelerator ring. This represents
    about 25 of the total budget.

21
TSR gt ELENA ?
  • Proposed ELENA/TSR lattice

22
THANK YOU
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