Impact of ILC Tracker Design on e + e - H 0 Z 0 m + m - X Analysis

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Impact of ILC Tracker Design on e e H 0 Z 0 X Analysis Hai-Jun Yang & Keith Riles University of Michigan, Ann Arbor ALCPG Workshop at Fermilab

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Impact of ILC Tracker Design on e + e -  H 0 Z 0  m + m - X Analysis. Hai-Jun Yang & Keith Riles University of Michigan, Ann Arbor ALCPG Workshop at Fermilab October 22-26 , 200 7. Physics Motivation. - PowerPoint PPT Presentation

Transcript of Impact of ILC Tracker Design on e + e - H 0 Z 0 m + m - X Analysis

Page 1: Impact of ILC Tracker Design on e + e -    H 0 Z 0    m + m - X Analysis

Impact of ILC Tracker Design onee H0Z0 X Analysis

Hai-Jun Yang & Keith RilesUniversity of Michigan, Ann Arbor

ALCPG Workshop at FermilabOctober 22-26, 2007

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10/25/2007 H.J. Yang - H-->mumu update 2

Physics MotivationTo determine a suitable ILC SiD tracker

momentum resolution capable of making a direct measurement of ee H0Z0 X

Small BRH

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10/25/2007 H.J. Yang - H-->mumu update 3

Cross Section of HZ X

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10/25/2007 H.J. Yang - H-->mumu update 4

MC Generator & Analysis Tool ee H0Z0 X

– Based on ILC350 beam setup– Polarization of e is -85%, eis 0– PandoraV2.3 (modified for H decay,

thanks to Michael E. Peskin) and PythiaV3.3– Java Analysis Studio V2.2.5– SDMar01, Fast MC Simulation and 1000 fb-1

– Track momentum resolution for SDMar01 (1/pt) = (2*10-5)2 + (7*10-4/pt/sin)2

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10/25/2007 H.J. Yang - H-->mumu update 5

Monte Carlo Samples• Signal – 10K: ee H0Z0 X

– MH=100, 110, 120, 130, 140, 150 GeV– Cross sections are 51, 46, 38, 27, 16, 7 ab, respectively. – Expected counts are 51, 46, 38, 27, 16, 7 for 1000 fb-1

• Background ee Z0Z0 X – 100 K, 31.6 fb• Background ee W+W – 400 K, 149.68 fb• Background ee Z/ - 500K, 2574.0 fb• Background ee Z - 400K, 416.3 fb• Background ee ZH

– MH=100, 110, 120, 130, 140, 150 GeV– 10K events for each Higgs mass point

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10/25/2007 H.J. Yang - H-->mumu update 6

Preselection Cuts• “Good”

– a) P > 20 GeV

– b) |cos | < 0.8

• At least 2 “Good”

• Eff_signal ~ 62.4% – 65%

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10/25/2007 H.J. Yang - H-->mumu update 7

Selection Cuts (MH=100 GeV)Opening angle between two Polar angle of two

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10/25/2007 H.J. Yang - H-->mumu update 8

Selection Cuts (MH=120 GeV)Opening angle between two Polar angle of two

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10/25/2007 H.J. Yang - H-->mumu update 9

Selection Efficiency

Lower efficiency for higher Higgs mass, which is mainly caused by wider opening angle between decay from Higgs.

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10/25/2007 H.J. Yang - H-->mumu update 10

M vs Track Momentum Resolution

MH=100 GeV MH=120 GeV

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10/25/2007 H.J. Yang - H-->mumu update 11

Signal Events - Detection Significance

The Hsignificance is improved with better track resolution.

Optimize Higgs significance for each Higgs mass point.

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10/25/2007 H.J. Yang - H-->mumu update 12

Branching Ratio UncertaintyThe detection significance improves significantly with improved momentum resolution, but branching ratio of H improves only modestly.

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10/25/2007 H.J. Yang - H-->mumu update 13

Higgs Mass Resolution

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10/25/2007 H.J. Yang - H-->mumu update 14

Higgs Mass Resolution

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10/25/2007 H.J. Yang - H-->mumu update 15

Higgs Mass ResolutionBetter Higgs mass resolution with better track resolution.

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10/25/2007 H.J. Yang - H-->mumu update 16

Preliminary ConclusionsThe SD tracker with nominal track momentum

resolution makes it possible but still hard to measure eeH0Z0 X.

But the direct measurement is feasible (>5 sigma for light Higgs mass ~ 100-140GeV) if the track momentum resolution is improved by a factor of ~ 2 or more.