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Funneling ps and ms

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Bruno Autin, Peter Sievers, Andr Verdier. CERN. Fran ois M ot. CEA, Saclay. 9/22/09. NuFact03, June 04 -11, New York Funneling pions and muons. 2. Proton Beam ... – PowerPoint PPT presentation

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Title: Funneling ps and ms


1
Funneling ps and ms
  • Bruno Autin, Peter Sievers, André Verdier
  • CERN
  • François Méot
  • CEA, Saclay

2
Proton Beam Parameters
3
Why a funneling system?
  • No exotic and expensive technology.
  • Lifetime in excess of one year.
  • Evolutionary design.

4
How it works?
  • The proton beam is switched to 4 targets in
    sequence.
  • Each of the 4 pion lines contains an integrated
    system of target, magnetic horn and cooling.
  • The funnel is made of large aperture magnets with
    quadrupolar and pulsed dipolar coils.

5
Funneling step by step
6
Magnetic horn
7
Horn Parameters
8
Target in Horn
9
Target dynamics 1
  • Condition for shock
  • Energy deposited in a time short wrt sound
  • propagation time. Typical scales
  • Distance 1 cm, vs 3000 m/s, ts 3 ms.
  • Synchrotron bunch length 5 ns
  • Accumulator pulse length 1 km 3 ms.
  • Escape from shock
  • Fragment the target Distance 1 mm, ts 0.3
    ms.
  • Good for accumulator. Insufficient for
    synchrotron.

10
Target dynamics 2
  • Condition for rupture (P. Drumm et al., nFact00)
  • Stress induced by shock exceeds elastic limit of
  • target material. Typical scales
  • Ds E a DT 3500 MPa at 10 Hz in Ta
  • Elastic limit 400 MPa at room temperature.
  • Escape from rupture
  • No shock, no stress.
  • Reduce DT by increasing repetition frequency and
  • beam size.

11
Effect of funneling on target parameters


Ttarget THelium
1 target
4 targets
12
Pion Beam Parameters
13
Polarities
Scheme 1 AC quadrupoles Scheme 2 DC
quadrupoles Good transmission. Reduced
transmission (2/3). Complicated power supplies
due Conventional power supplies. to high stored
magnetic energy.
14
Optical functions
Center of mass trajectory b-functions
15
Magnet Parameters
16
Muon production
  • Y Nm/Np versus longitudinal emittance for
  • two transverse admittances et 1p cm (no
    cooling), 4p cm (cooling)
  • three regimes solenoid, conventional and high
    field quadrupoles.

17
Conclusions
  • Muon production for neutrino factories is on the
    way of being solved within the context of low
    energy, high repetition frequency proton driver.
  • Target and horn developments have started but not
    at the wanted pace.
  • Pending topics magnet design, proton dump.
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