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Low Q option of ILC

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Tsep (ns) 5640. 2820. 2820. Nb/train. 1.0e 10. 2.0e 10. 2.0e 10. Ne/bunch. 500. ECM (GeV) Low Q ... Advantages of Low Q option. Same Luminosity but less bunch ... – PowerPoint PPT presentation

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Title: Low Q option of ILC


1
Low Q option of ILC
  • 2005.June 8
  • Y. Sugimoto, T. Fujikawa

2
Main MDI Issues
  • Crossing angle
  • L
  • Beam parameters
  • Ne/bunch
  • s
  • Timing
  • etc.
  • BCAL
  • All sub-det.
  • Solenoid, TPC
  • BCAL
  • All sub-det.
  • Minimum veto angle
  • n, e/e- back scattering
  • Anti-solenoid
  • DID
  • Event overlap
  • Background in BCAL
  • Readout timing

MDI issues are Physics/Detector issues!
3
Parameter sets by Tor Raubenheimer
peak luminosity
  • TESLA
  • USSC
  • Nominal
  • Low Q (Low charge)
  • Large Y (Large Emittance)
  • Low P
  • High Lum

3?1034
parameterspace
2?1034
Nick Walker (LCWS2005)
4
Proposed Machine Parameters
TESLA Nominal Low Q
ECM (GeV) 500 500 500
Ne/bunch 2.0e10 2.0e10 1.0e10
Nb/train 2820 2820 5640
Tsep (ns) 335.9 307.7 153.8
bx (m) 1.5e-2 2.1e-2 1.2e-2
by (m) 4.0e-4 4.0e-4 2.0e-4
sx (m) 5.54e-7 6.55e-7 4.95e-7
sy (m) 5.0e-9 5.7e-9 3.5e-9
sz (m) 3.0e-4 3.0e-4 1.5e-4
PBeamstrahlung (W) 3.35e5 2.48e5 2.05e5
L (cm-2 s-1) 2.94e34 2.03e34 2.01e34
Incoherent pair/BX 4.14e5 2.59e5 0.84e5
5
Advantages of Low Q option
  • Same Luminosity but less bunch Luminosity (1/2 of
    nominal option)
  • Less possibility of event overlap (2-g events)
  • Less beamstrahlung power
  • Less incoherent pair background
  • Per BX 1/5 of TESLA design, 1/3 of nominal
    option
  • Less b.g. hits in the Beam Calorimeter ? Better
    veto efficiency
  • Per Train 2/5 of TESLA design, 2/3 of nominal
    option
  • Less b.g. hits in the Vertex Detector

6
Disadvantages(?) of LowQ option
  • Smaller beta functions and beam size
  • Compatible with large l ?
  • Smaller bunch spacing of 154 ns
  • Hard job of the Damping Ring
  • No problem for FPCCD
  • How about other detector components?

7
Simulation Study
  • Pair background hit rate on the 1st layer of the
    Vertex Detector (R24mm)
  • Simulation using CAIN and JUPITER
  • Hit rate of the Low Q option is 1/3 of the
    nominal option, as expected

8
Summary
  • New ILC parameter sets are different from that of
    TESLA design
  • LowQ option is attractive from the view point of
    the detector
  • It has been confirmed by simulation study using
    CAIN and JUPITER that the LowQ option makes less
    background hits on the vertex detector than the
    nominal option
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