Plan for the muon detector and the toroid system simulation - PowerPoint PPT Presentation

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Plan for the muon detector and the toroid system simulation

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Doris Y. Kim, UIUC. 1. Plan for the muon detector and the toroid system simulation. Content ... For the sake of coming TDR, simplify as much as possible. Geometry ... – PowerPoint PPT presentation

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Title: Plan for the muon detector and the toroid system simulation


1
Plan for the muon detector and the toroid system
simulation
  • Content
  • What we want to do
  • Design Update.
  • Toroid.
  • Muon Trigger.
  • Current MC Situation.
  • Man-power.
  • Plan.
  • Doris Y. Kim
  • UI Urbana-Champaign.
  • For the sake of
  • March 28, 1999
  • BTeV Meeting

2
What we want to do Design Update.
  • The design of the muon system is changed since
    last TDR.

m1
m2
m3
Station 0 omitted. Nominal IP constraint instead
of (m0, m1) Shielding vs. Toroid?
3
Design Update vs Resolution
  • Analytic study by Jim Wiss.
  • f 90, 0, 270 degrees
  • One vs. two toroids
  • 2 (m2, m3 ) vs. 3 (m1 m2 m3) stations.
  • Nominal beam center constraint is used.
  • Assumed rms spatial res 2.5mm.
  • Interference between dipole and toroidal fields
    is reduced with 2 toroids instead of 1.
  • With 2 toroids, res. difference between 2 and 3
    station cases is small, but this is ideal
    situation.

4
Toroid
  • Study by Chuck Brown.
  • Thickness of toroid 34, 51, 68 inches?
  • Shape not final Octagonal or Box?

CERN POISSON
5
Muon Trigger Requirement
  • 1st level With nominal beam spot constraint r
    information from the last two stations (within
    the same f segment), achieve dimuon Pt trigger.
  • Also, from the detachment information from
    silicon detector, try single muon trigger.

6
Current Situation of the muon system simulation.
  • In Mcfast
  • Considerable material in event generation, the
    silicon tracking system and the calorimeter
    system.
  • But just skeleton of the muon system.
  • Geometry is not correct For each arm, two
    tube-shaped iron absorbers instead of toroids,
    etc.
  • No muon trigger simulation in both 1st
    (stand-alone) and higher levels (conjunction with
    other detectors).
  • No p punch-through coming in from the
    calorimeter side simulated, even though the
    effect for the upmost station will be huge.
  • No delta-ray simulation.

7
Man-Power / Division of Labor.
  • Geometry, delta-ray
  • Trigger
  • p punch-through
  • Doris Kim (UIUC)
  • Kevin Stenson (Vanderbilt)
  • Weijun Xiong (Puerto Rico)

8
Plan / How we will proceed.
  • For the sake of coming TDR, simplify as much
    as possible.
  • Geometry
  • Put two ideal toroids (1.5 T) each arm B(r) in
    f direction.
  • Put stainless-steel muon stations with a varying
    inner radius.
  • Put aluminum shields to reset delta-rays.
  • p punch-through
  • Parameterize no. and position of particles from
    punch-through, either by measurement or detailed
    simulation (Geant) information.
  • Search for the best geometry of the absorber.
  • Getting preliminary results now, any suggestions
    welcome.

9
Plan for Trigger Simulation
a delta-ray faking high energy muon
  • Effect of Delta-rays
  • Trigger
  • (Noise) delta-rays p punch-through simulation
    will be in.
  • 2 vs 3 stations scenario will be revisited. (see
    plot.)
  • Current strategy Ideal track smearing
    efficiency reduction.

toroid
(toroid)
low energy muon
m1
m2
m3
m1 station as a discriminator?
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