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The charged Higgs boson at LEP Towards the final combination Pierre Lutz (Saclay)

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Presentation on theme: "The charged Higgs boson at LEP Towards the final combination Pierre Lutz (Saclay)"— Presentation transcript:

1 The charged Higgs boson at LEP Towards the final combination Pierre Lutz (Saclay)

2 1/06/2007 LCWS07 DESY / Pierre Lutz 2 A preliminary combination occured for the summer 2001 conferences. A preliminary combination occured for the summer 2001 conferences. Since then, the 4 expts have finalized their results : Since then, the 4 expts have finalized their results : (ALEPH 2002, L3 2003, DELPHI 2004 and OPAL hopefully soon) (ALEPH 2002, L3 2003, DELPHI 2004 and OPAL hopefully soon) It’s time to go a step forward just before the final words on this subject from LEP It’s time to go a step forward just before the final words on this subject from LEP

3 1/06/2007 LCWS07 DESY / Pierre Lutz 3 Introduction Charged Higgs boson (H 6 ) : colorless, spinless, electrically charged particle. Charged Higgs boson (H 6 ) : colorless, spinless, electrically charged particle. INSTANT EVIDENCE OF PHYSICS BEYOND THE STANDARD MODEL INSTANT EVIDENCE OF PHYSICS BEYOND THE STANDARD MODEL Appears in any Two-Higgs-Doublet Models (2HDM) Appears in any Two-Higgs-Doublet Models (2HDM)

4 1/06/2007 LCWS07 DESY / Pierre Lutz 4 Basics (e + e - -> H + H - ) = k(1-4m 2 H /s) 3/2 (e + e - -> H + H - ) = k(1-4m 2 H /s) 3/2 (ew)radiative corrections are small (~5%) (ew)radiative corrections are small (~5%) Decay modes : cs, tn and W*A Decay modes : cs, tn and W*A Branching fractions depend on type of Branching fractions depend on type of 2 Higgs Doublet Model (2HDM) 2 Higgs Doublet Model (2HDM) Dominant background : W pairs Dominant background : W pairs

5 1/06/2007 LCWS07 DESY / Pierre Lutz 5 List of available searches # samples 22 43 12 45

6 1/06/2007 LCWS07 DESY / Pierre Lutz 6 2HDM type II One Higgs doublet provides masses for up-type quarks, the other for down-type quarks (~MSSM) One Higgs doublet provides masses for up-type quarks, the other for down-type quarks (~MSSM) For large A masses, or |log(tanb)| > 1, only cs and tn channels contribute. For large A masses, or |log(tanb)| > 1, only cs and tn channels contribute.

7 1/06/2007 LCWS07 DESY / Pierre Lutz 7 2HDM type II (cont ’d.) (Historical) assumption : the cs and tn channels exhaust the H + decay width. (Historical) assumption : the cs and tn channels exhaust the H + decay width. Plots are B(H + -> tn ) vs H + mass. Plots are B(H + -> tn ) vs H + mass. cs  low tan b cs  low tan b tn  high tan b tn  high tan b

8 1/06/2007 LCWS07 DESY / Pierre Lutz 8 2HDM type II : ALEPH final 2HDM type II : ALEPH final Small data excess in leptonic and small deficit in hadronic channel Note the (observed) exclusion beyond the W mass in the hadronic channel

9 1/06/2007 LCWS07 DESY / Pierre Lutz 9 2HDM type II : DELPHI final Note a small excess in the mixed channel Small deficit

10 1/06/2007 LCWS07 DESY / Pierre Lutz 10 2HDM type II : L3 final Almost perfect agreement between observation and expectation

11 1/06/2007 LCWS07 DESY / Pierre Lutz 11 2HDM type II : final results

12 1/06/2007 LCWS07 DESY / Pierre Lutz 12 2HDM type II : combination Contours based on the observed p-values CL b 3 zones show an excess above 2 s, far from the expected limit

13 1/06/2007 LCWS07 DESY / Pierre Lutz 13 2HDM type II : combination Obs. exclusion @ 99.7% Obs. exclusion @ 95% Expected excl. @ 95% Small overall excess in the mixed channel. Preliminary Exclusion limit > mW nearly everywhere

14 1/06/2007 LCWS07 DESY / Pierre Lutz 14 2HDM type II : combination Contribution of the 3 channels separately mW

15 1/06/2007 LCWS07 DESY / Pierre Lutz 15 2HDM type II : combination 95% CL bound on x-sect., for 4 B(H  tn ) The values of mW used in background simulations has a strong impact on the limits.

16 1/06/2007 LCWS07 DESY / Pierre Lutz 16 2HDM type I One Higgs doublet provides masses to all (up- and down-type) quarks (~SM) One Higgs doublet provides masses to all (up- and down-type) quarks (~SM)

17 1/06/2007 LCWS07 DESY / Pierre Lutz 17 2HDM type I (cont ’d.) Need a scan in a 3-dim space : m H +,m A, and tan b Need a scan in a 3-dim space : m H +,m A, and tan b Conservatively, when there was an overlap between 2 channels, the one with the lowest expected sensitivity was ignored to avoid double counting Conservatively, when there was an overlap between 2 channels, the one with the lowest expected sensitivity was ignored to avoid double counting W*AW*A and cscs as an exemple W*AW*A and cscs as an exemple

18 1/06/2007 LCWS07 DESY / Pierre Lutz 18 2HDM type I : combination Contours based on the observed p-values CL b Excess (< 3 s ) in the W*A regions, for low and intermediate A masses

19 1/06/2007 LCWS07 DESY / Pierre Lutz 19 2HDM type I : combination Observed 95% CL limits Expected Pure fermionic decays Pure bosonic decays

20 1/06/2007 LCWS07 DESY / Pierre Lutz 20 2HDM type I : combination Everywhere, the limit is found in a region where an excess is observed : So, there is a systematic shift (~3 GeV) between obs. and expect.

21 1/06/2007 LCWS07 DESY / Pierre Lutz 21 Conclusions Still preliminary, but nearly final. Still preliminary, but nearly final. In the historical scenario (2HDM type II like) with fermionic decay channels alone In the historical scenario (2HDM type II like) with fermionic decay channels alone m H > 80.1 GeV m H > 80.1 GeV (limited by WW background and W mass) (limited by WW background and W mass) NEW ! Exploration for a 2HDM type I (with mA > 12 GeV) NEW ! Exploration for a 2HDM type I (with mA > 12 GeV) m H > 76.1 GeV m H > 76.1 GeV due to a slight excess w.r.t. the expectation due to a slight excess w.r.t. the expectation

22 1/06/2007 LCWS07 DESY / Pierre Lutz 22 Lessons for the future We noticed too late that the expts have chosen different W mass in their simul. We noticed too late that the expts have chosen different W mass in their simul. (A : 80.45 ; D : 80.40 ; L3 : 80.356 ; O : 80.33) (A : 80.45 ; D : 80.40 ; L3 : 80.356 ; O : 80.33) It is impossible to correct for that ! It is impossible to correct for that ! Overlapping channels should be treated with care, in order to avoid the (perhaps too) conservative approach used here. It would have been possible here with an explicit anti- btag in the cs channel Overlapping channels should be treated with care, in order to avoid the (perhaps too) conservative approach used here. It would have been possible here with an explicit anti- btag in the cs channel


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