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Measurement the Higgs mass via the channel: e + e - → Z H → e + e - + X & Analog vs. Digital Energy Reconstruction in the Si-W ECal Youssef KHOULAKI ILCP.

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Presentation on theme: "Measurement the Higgs mass via the channel: e + e - → Z H → e + e - + X & Analog vs. Digital Energy Reconstruction in the Si-W ECal Youssef KHOULAKI ILCP."— Presentation transcript:

1 Measurement the Higgs mass via the channel: e + e - → Z H → e + e - + X & Analog vs. Digital Energy Reconstruction in the Si-W ECal Youssef KHOULAKI ILCP Meeting, CERN – Genève, 25/10/2010

2 ILC & ILD 25-Sep-102Y.khoulaki

3 25-Sep-10Y.khoulaki3 Detection of the Higgs boson from its production mechanism (Simulations) The H observation does not dependent on its decay mode Response provided whatever the scenario The H recoil mass is given by:

4 Parameters in simulations 25-Sep-10Y.khoulaki4 ILD_00 detector: M H = 120 GeV  s = 250 GeV e + polarization = 30% e - polarization = 80% L= 250 fb -1 Background: - SM events with 2 and 4 fermions including e+e- Identification of the Z boson: - Selection of the e+e- pair which gives the best mass for the Z boson : MZ reconstructed = MZ ± 10 GeV - Central leptons : |cos(  i)| < 0.9 - Opposite charges

5 25-Sep-10Y.khoulaki5 Event selection ( Cuts on kinematic variables) If you cannot see the values of the cuts, go on to the Backup slides

6 25-Sep-10Y.khoulaki6 Reconstruction of the Higgs recoil mass Signal measurement: Function Gaussian Peak Exponential Tail: Background measurement: Fitted by a polynomial sum Polarization mode (+,-)

7 25-Sep-10Y.khoulaki7 Reconstruction recoil mass Polarisation (30%, 80%) (+,-)(-,+) Signal seulSignal + BDFSignal seulSignal + BDF 120.486 ± 0.073120.368 ± 0.100120.507 ± 0.085120.445 ± 0.110 0.638 ± 0.0510.0575 ± 0.0830.654 ± 0.0620.592 ± 0.100 Presentation and proceedings at: International Linear Collider Workshop 2010 (LCWS10 & ILC10), Beijing : China, « Measurement of the Higgs mass via the channel » Y. Khoulaki, D. Benchekroun, L. Morin, J.Y. Hostachy http://arxiv.org/abs/1006.1241

8 Analog and Digital Energy reconstruction Data : Energy reconstruction : N i : Number of hits in the compartment i (i=1,2,3) 8Y.khoulaki25-Sep-10

9 With experimental data Ehit > 0.5 MIPs (standard reconstructed data) Y.khoulaki25-Sep-109 Ehit > 0.5 MIPs  Linear behavior at low energy  Digital method better for E<2 GeV : Landau fluctuations CALICE Analysis Phone Meeting, November 10th 2008 « Comparison of analog and digital energy measurements using DESY-2006 data » D. Benchekroun, Y. khoulaki http://ilcagenda.linearcollider.org/getFile.py/access?contribId=3&resId=0&materialId=slides&confId=3024

10 New REC. DATA (without threshold ) Initializing the threshold : CALICE RAW2CALOHIT package //... _signalThreshold = 0.; // … New DESY Rec. Data: Our the results can be found at the addresses: 1 GeV : /grid/calice/users/khoulaki/tb-desy/My_REC_without_threshold/ Run230098_rec_kh.000.slcio 2 GeV : /grid/calice/users/khoulaki/tb-desy/My_REC_without_threshold/ Run230099_rec_kh.000.slcio 3 GeV : /grid/calice/users/khoulaki/tb-desy/My_REC_without_threshold/ Run230100_rec_kh.000.slcio 4 GeV : /grid/calice/users/khoulaki/tb-desy/My_REC_without_threshold/ Run230101_rec_kh.000.slcio 5 GeV : /grid/calice/users/khoulaki/tb-desy/My_REC_without_threshold/ Run230104_rec_kh.000.slcio 6 GeV : /grid/calice/users/khoulaki/tb-desy/My_REC_without_threshold/ Run230248_rec_kh.000.slcio  The thresholds are defined by hand during the analysis Y.khoulaki25-Sep-1010

11 Linearity and Resolution for different thresholds 0 MIPs ≤ E hit ≤O.2 MIPs 0.4 to 1 MIPs 0.3 MIPs Y.khoulaki25-Sep-1011 - Same behavior for all energies - Better resolution around 0.2 – 0.3 MIPs E hit > 0.3 MIPs : E < 5 GeV E hit > 0.4 MIPs : E < 3 GeV

12 Y.khoulaki Methoda(%)C(%) Analog16.311.62 Analog + Digital (0.4 MIPs)15.671.84 25-Sep-1012 - E < E cross : resolution taken from digital - E > E cross : resolution taken from analog

13 Y.khoulaki Data – MC Comparison (Number of hit Cells vs. Energy ) 25-Sep-1013 - Digitization of MC done using a simple processor (from D. Ward) - No noise added to the non-hitted cells Red : MC Blue : DATA

14 Y.khoulaki Energy resolution vs. Thresholds (Comparison between the DESY data (in Red) and the MC predictions (in blue)) 25-Sep-1014

15 Conclusion for the Analog/Digital Part Digital method can give better resolution using lower thresholds (0.3 -0.4 MIPs) Results to be confirmed by MC simulations ( for the E hit > 0.4 MIPs) Next steps : digitization MC (with K. Krastev, LPSC) Simulations for 5x5 mm 2 detection pads Y.khoulaki25-Sep-1015 CALICE Collaboration meeting at Casablanca, September 22-24, 2010 «Analog vs. Digital Energy Measurement in the ECAL » Y. Khoulaki Y. Khoulaki, D. Benchekroun http://ilcagenda.linearcollider.org/getFile.py/access?contribId=11&sessionId=3&re sId=0&materialId=slides&confId=4776

16 BACKUP SLIDES Y.khoulaki25-Sep-1016

17 Event selection (cuts on kinematic variables) 25-Sep-10Y.khoulaki17

18 Y.khoulaki25-Sep-1018 Total Number of hits for different Energy ( MC Prediction) Slide 6

19 Total Number of hits for different thresholds ( MC Prediction) Y.khoulaki25-Sep-1019

20 Resolution for different thresholds ( DESY DATA) Y.khoulaki25-Sep-1020

21 Y.khoulaki25-Sep-1021 Resolution for different thresholds ( MC Prediction)


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