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Summary of the FCAL Workshop Cracow, February 12-13

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Presentation on theme: "Summary of the FCAL Workshop Cracow, February 12-13"— Presentation transcript:

1 Summary of the FCAL Workshop Cracow, February 12-13
Ch.Grah HH-Zeuthen Meeting 2nd March 2006

2 FCAL Meeting Overview FCAL collaboration meeting February at the Institute of Nuclear Physics PAN, Cracow 30 participants from 8 nations Will cover the luminosity and simulation part in this presentation. W.Lange on electronics/DAQ/sensors HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

3 Reminder of the FCAL Region
BeamCal: 4 < θ < 28 mrad IP PhotoCal (>100m) PhotoCal: 0.1 < θ < 0.4 mrad LumiCal: 26 < θ < 82 mrad HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

4 Measure Luminosity – Physics Background
M.Pandurovic Simulation of Physics Background for Luminosity Calorimeter Bhabha generator: BHLUMI integrated into Detector simulation: BARBIE V4.1 Background generator: WHIZARD V1.40 Background are e+e  e+e- l+l- (l=e,μ) four-lepton events x [cm] y [cm] B/S: 5·10-5 ‘1’,2,4 cuts’ B/S: 4·10-4 HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

5 Measure Luminosity - Systematics
C.Rimbault The impact of electromagnetic deflection due to beam-beam effect on Bhabha scattering e- e+ e+ e-  focusing of ~0.04 mrad HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

6 Bhabha deflection NBh bef. def. = 35986 NBh added by def. = 4 NBh suppressed by def. = 132 q0 before deflection q1 after deflection Difference between theoretical and “real” nb of Bhabhas : -0.36% “Bhabha suppression effect” HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

7 Measure Luminosity - Systematics
A.Sapronov Systematic effects on luminosity measurements at 2 and 20 mrad beam crossing angles x y dr qoft dr = 400 mm qft(-p;p) HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

8 Findings A.Sapronov Systematic effects on luminosity measurements at 2 and 20 mrad beam crossing angles Comparing the systematic effects due to LumiCal inner radius deviation, radial beam offset and LumiCal tilt we see: - the effects are comparable ( or a little bit larger) at 20 mrad with respect to 2 mrad, for the case when LumiCal is centered around the outgoing beam pipe - the effects are dramatically larger (up to three orders of magnitude) if LumiCal is centered around the 'detector axis'. HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

9 Luminosity Measurement - Systematics
R.Ingbir Precison Luminosity Measurements Investigating: offsets (crosscheck with Sapronov) magnetic field influence bias resolution X (cm) HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

10 This is assuming knowing in perfect precision many parameters
Correction possible Before correction after correction Y (cm) N3 N1 N4 N2 But !!!!!! This is assuming knowing in perfect precision many parameters X (cm) HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

11 Detectors are centered around the outgoing beam
LumiCal Summary Recommendation for the geometry still hold true: Detectors are centered around the outgoing beam LumiCal rmin=13 cm rmax=28 cm (Reasonable Statistics) BeamCal rmin=2 cm rmax=16 cm + 30o blind area (incoming beam) HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

12 BeamCal Simulation A.Sapronov Beam parameters influence on spatial energy distribution in BeamCal Full Geant4 simulation with flexible geometry and segmentation (simplified Bfield). E = ΣElayer(i) Energy/Layer distribution 20mrad, DiD 20mrad, antiDiD HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

13 BeamCal Simulation C.Grah Fast Beam Diagnostics at the ILC Using the Beam Calorimeter single and double parameter analysis Quantity Nominal Value Precision 2mrad 20mrad 20mrad (2par) sx 553 nm 3.1 2.9 2.8 sx 5.2 7.4 7.6 sy 5.0 nm 0.3 0.2 sy 0.4 sz 300 mm 4.8 8.5 11.1 sz 3.7 6.3 εy 40x10-9mrad 1.7 4.2 4.1 4.7 Dx 17.7 9.3 10 Dy 0.5 0.6 N 2x1010 0.01 DN 0.02 0.03 ILCNOM, 20mrad DID Extrapolation of beamstrahlung pairs to BeamCal frontface. HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

14 More presentations from...
W. Lohmann General S.Jadach Lesson from Bhabha scattering calculations performed for LEP M. Karbowiak Preliminary studies of the systematic effects on theta angle reconstruction from deformed structure of LumiCal P.Mikes Preliminary results of LumiCal simulation B.Pawlik LumiCal simulation including sensors description J.Lukasik Simulation of the Bhabha events using Barbie package HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I

15 For more details and all talks, visit:
HH-Zeuthen, 2nd March 2006 Ch.Grah: FCAL Workshop Summary I


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