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Low Q option of ILC. 2005.June 8 Y. Sugimoto, T. Fujikawa. Crossing angle L* Beam parameters Ne/bunch s Timing etc. Minimum veto angle n, e+/e- back scattering Anti-solenoid DID Event overlap Background in BCAL Readout timing. Main MDI Issues. BCAL All sub-det. Solenoid, TPC
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Low Q option of ILC 2005.June 8 Y. Sugimoto, T. Fujikawa
Crossing angle L* Beam parameters Ne/bunch s Timing etc. Minimum veto angle n, e+/e- back scattering Anti-solenoid DID Event overlap Background in BCAL Readout timing Main MDI Issues • BCAL • All sub-det. • Solenoid, TPC • BCAL • All sub-det. MDI issues are Physics/Detector issues!
Parameter sets by Tor Raubenheimer peak luminosity • TESLA • USSC • Nominal • Low Q (Low charge) • Large Y (Large Emittance) • Low P • High Lum 31034 parameterspace 21034 Nick Walker (LCWS2005)
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
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?
Simulation Study • Pair background hit rate on the 1st layer of the Vertex Detector (R=24mm) • Simulation using CAIN and JUPITER • Hit rate of the Low Q option is ~1/3 of the nominal option, as expected
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