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Detector WG

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Good aspect ratio for small radius (compared to strips) Improves patter recognition robustness ... and smaller Bhabha pileup may change this conclusion. Muon ... – PowerPoint PPT presentation

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Title: Detector WG


1
Detector WG
  • Francesco Forti
  • SuperB Workshop
  • LNF, 16-18 March, 2006

2
A SuperB Detector
  • Basic conclusion from December Workshop
  • It is possible to reuse large parts of Babar and
    Belle with relatively minor technology changes
  • Detector components
  • Silicon vertex, with small radius pixels,
    essential for reduced boost.
  • Drift chamber
  • DIRC style PID, with improved readout
  • CsI(Tl) calorimeter in barrel, something faster
    (LYSO) in endcap
  • Existing coil
  • LST style muon detectors

3
Issue number 0
  • Beam parameters
  • Current and Collision frequency vary wildly in
    different designs
  • Was mA and 1MHz in december
  • Raimondi Round with extraction 100 mA and 10
    MHz
  • Raimondi Flat(3) uncompressed 1600mA and 500
    MHz
  • Seeman 4500 mA and 68 MHz
  • Different options have very large impact on
    technology choices and on the reusability of
    Babar and Belle components.

4
Collision frequency
  • With 0.1-1MHz fc one could exploit the beam
    crossing time structure to relax detector
    constraints
  • Drift time
  • Electronics shaping time
  • Crystal decay time
  • One the other hand a low fc implies overlapping
    events (mainly Bhabha)
  • The 10-50MHz regime is the LHC electronics area
  • It might be possible to exploit the bx time
    structure, but is it useful ?
  • At high fc (gt100MHz) back to current BFactories
    operation mode
  • Continuous beam, no bx information
  • no pileup

5
Current
  • Two consequences of higher currents
  • higher background in the detector
  • occupancy
  • radiation damage
  • power dissipation in the beampipe requires water
    cooling
  • more material
  • larger radius

6
Types and level of backgrounds
  • Beam gas
  • Synchroton radiation
  • ? Both proportional to current
  • Should not be a problem at Superb
  • They become a problem at higher currents
  • Luminosity sources (eg radiative Bhabhas)
  • Careful IR design. Bhabhas into the detector are
    there.
  • Beam-beam interactions
  • Potentially important
  • Touschek background
  • 1/E2. Improves with smaller asymmetry. But, much
    higher beam density
  • Thermal outgassing
  • Due to HOM losses. Not an issue with small
    currents
  • Injection background
  • Not an issue because of damping rings scheme
  • Maybe not true anymore with the 1 collision/turn
    scheme
  • Bursts
  • Due to dust. No real cure. Need robustness of
    detector

7
Background bottom line
  • Probably reasonable to assume background is not
    larger than what with have today
  • Cannot claim a large background reduction with
    present schemes
  • Need to design a robust detector with the enough
    segmentation and radiation hardness to withstand
    surprises (x5 safety margin)
  • IR design is critical
  • Radiative Bhabhas
  • Syncrotron radiation shielding
  • Shielding from beam-beam blow up

8
Issue number 1
  • Boost
  • lower boost advantegeous for machine design
  • Babar 9 3.1 ß?0.56
  • Belle 8 3.5 ß?0.45
  • SuperB? 7 4 ß?0.28
  • we can afford to have a lower boost only if the
    vertexing resolution is good
  • small radius beam pipe
  • very little material in b.p. and first layer
  • if not, then we should stay with higher boost
    (0.45)

9
Separation significance
  • ltDzgt/s(Dz) vs bg

10
Detector components
  • Vertexing
  • Thin pixel layer glued on beam pipe
  • Good aspect ratio for small radius (compared to
    strips)
  • Improves patter recognition robustness
  • needs RD
  • Intermediate tracking
  • Strip detectors
  • More or less like the current detectors
  • Reduction in thickness would be desirable, but
    not essential
  • Central tracking
  • Drift chamber
  • Solid state tracking not performant at low
    momentum
  • Need to optimize cell size against occupancy
  • Belle has developed a fast gas small cell DCH,
    but with a degraded resolutions

11
Detector components
  • PID
  • Cerenkov based PID like DIRC
  • Need development on readout
  • Fast focusing DIRC
  • TOP
  • Endcap region requires special study
  • Calorimeter
  • Barrel part could be reused (see other talks)
  • In the endcaps require smaller Moliere radius and
    faster crystals ? LYSO
  • Higher currents and smaller Bhabha pileup may
    change this conclusion
  • Muon
  • It doesnt seem to be a problem
  • Trigger/DAQ
  • Calorimeter and/or tracking information
  • Not substantially different from current schemes.
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