Download presentation
Presentation is loading. Please wait.
Published byRichard Poole Modified over 9 years ago
1
Alex Melnitchouk DPF conference - May 2002 1 Search for Fermiophobic Higgs in the h Channel DPF 2002, Williamsburg Alex Melnitchouk (Brown University) on behalf of D0 Collaboration
2
Alex Melnitchouk DPF conference - May 2002 2 Fermiophobic Higgs. Theoretical Outlook Many of SM extensions predict enhanced rate for Higgs decay into photon pairs due to suppressed couplings to - light quarks, - heavy quarks (TopColor) - up-type fermions (MSSM+smth) - all fermions Enhanced rate is also predicted by some models that employ Extra Dimensions as well as other Exotic models.
3
Alex Melnitchouk DPF conference - May 2002 3 Fermiophobic Higgs. Experimental Outlook From Experimental Point of View it is convenient to consider decays of the Higgs in two extreme cases: 1. all fermion couplings are zero (Fermiophobic Higgs) 2. Top Quark coupling is allowed (Topcolor Higgs)
4
Alex Melnitchouk DPF conference - May 2002 4 Enhancement of h decays h Branching Ratio Higgs Mass Standard Model Fermiofobic Higgs some other non SM predictions in general we should be prepared for any Br(h ) due to new physics - quote S.Mrenna, J.Wells (hep-ph/0001226)
5
Alex Melnitchouk DPF conference - May 2002 5 Why Look for Fermiophobic Higgs at Fermilab ? Tevatron performance offers search possibilities beyond current mass limits within next few years In comparison with LEP there is additional possibility of Higgs production via gluon fusion also TopColor Higgs can be looked for D0 is working on WW and channels Both analyses rely mostly on the calorimeter (most understood of all D0 sub-detectors) Comparative Advantages : WW is predicted to have higher Branching ratio is a clean signature, has smaller backgrounds
6
Alex Melnitchouk DPF conference - May 2002 6 Cross-Sections of Signal Production. Final States Major final states are : - - or more jets t 80 100 120 140 160 0.01 0.1 1.0 10.0 Higgs Mass Cross-Section, pb -1 W (Z) g g t h q q h q q h Production Processes: gluon fusion, W/Z associated, W/Z fusion
7
Alex Melnitchouk DPF conference - May 2002 7 Background Cross Sections 100 125 150 180 0.1 0.01 0.001 0.0001 jj jj total QCD M d /d M pb -1 /GeV Major Backgrounds are QCD processes that in the final state contain : - two real photons - one real photon and a hadronic jet that fakes a photon - two hadronic jets faking photons
8
Alex Melnitchouk DPF conference - May 2002 8 Previous Results RunI (0.1 fb -1 ) D0 : 2 jets analysis found 4 events (expected background = 6.0 +/-2.1 ) set mass limit of 78.5 GeV at 95% C.L. CDF : 2 jets; e, , MissingEt analysis found 6 events (expected background = 6.2 +/-2.1 ) set mass limit of 82 GeV at 95% C.L. LEP limit : 108.2 GeV at 95% CL
9
Alex Melnitchouk DPF conference - May 2002 9 Tevatron RunII Sensitivities (gluon fusion not included) G.Landsberg and K.Matchev(hep-ex/0001007) estimated Tevatron RunII limits on h Branching Ratio as a function of Higgs Mass with 95%CL 100 120 140 160 180 Higgs Mass 0.01 0.02 0.05 0.1 0.2 0.5 Br(h RunI (0.1 fb -1 ) RunIIa (2.0 fb -1 ) RunIIb (30 fb -1 ) Fermiophobic h Preliminary LEP exclusion contour, A Andre Sopczak(hep-ph/0112082)
10
Alex Melnitchouk DPF conference - May 2002 10 Tevatron RunII Sensitivities (gluon fusion included) 100 120 140 160 180 Higgs Mass 0.01 0.02 0.2 0.05 0.1 0.5 h Branching Ratio RunI (0.1 fb -1 ) RunIIa (2.0 fb -1 ) RunIIb (30 fb -1 ) MSSM+smth h
11
Alex Melnitchouk DPF conference - May 2002 11 Something about Photon ID specifics? Not sure what to put for this
12
Alex Melnitchouk DPF conference - May 2002 12 Selection of Candidate Events Trigger: diEM or Single EM high Pt triggers Kinematic cuts: Pt >20GeV Acceptance cuts: Central Calorimeter (CC) (| |<1.1) or EndCap Calorimeter (EC) (1.5<| |<2.4), away ( 0.015) from -cracks in CC Photon ID: -0.05<Isolation<0.1, 0.95<Emfraction<1.05, shower shape consistent with EM shape (8x8 Hmatrix 2 <75), total Pt (within | |<0.1) of tracks <1.46 GeV
13
Alex Melnitchouk DPF conference - May 2002 13 Monte Carlo Estimate of h X Efficiencies W/Z associated W/Z fusiongluon fusion M=100 60.5 +/- 0.762.6 +/- 0.760.6 +/- 0.7 120 63.0 +/- 0.764.6 +/- 0.762.4 +/- 0.7 150 64.0 +/- 0.766.3 +/- 0.764.0 +/- 0.7 200 62.5 +/- 0.767.3 +/- 0.766.0 +/- 0.7 250 58.5 +/- 0.767.2 +/- 0.764.8 +/- 0.7 300 52.0 +/- 0.768.3 +/- 0.7 Included : ID (without 2 cut ), Acceptance NOT included : Kinematic cuts
14
Alex Melnitchouk DPF conference - May 2002 14 Signal and Background Monte Carlo Distributions = (E( 1) - E( 2)) / (E( 1) + E( 2)) (Some or all of these (if any) as they are or remade for double-checking their validity)
15
Alex Melnitchouk DPF conference - May 2002 15 di-EM Invariant Mass from 11/01-04/02 D0 data estimated background contribution from direct tight and loose cuts (calorimeter info only) Isolated Candidate Events + tracking info Aslo need to calculate other QCD backgrounds, (and Z?)
16
Alex Melnitchouk DPF conference - May 2002 16 Other plots ? In case there are any suggestions
17
Alex Melnitchouk DPF conference - May 2002 17 Event Display of Candidate (or jet) ? Do you think it is worth to pick a most “ h->gamma gamma looking ” event out of the mass distribution two slides ago and show various event displays of it?
18
Alex Melnitchouk DPF conference - May 2002 18 Conclusions …
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.