1. Standard Model Higgs Searches at the Tevatron (Low Mass : M H  ~140 GeV/c 2 ) Kohei Yorita University of Chicago The XLIIIrd Rencontres de Moriond EW La Thuile in Italy, March 1 - 8, 2008 For the CDF and D ø Collaborations

2. ContentsContents March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p2/18 i. Tevatron, CDF/D ø, SM Higgs ii. Search Results > H  bb > H  bb - WH  l bb (CDF(1.9fb -1 )/D  (1.7fb -1 )) - WH  l bb (CDF(1.9fb -1 )/D  (1.7fb -1 )) - ZH  l + l - bb (CDF(1.0fb -1 )/D  (1.1fb -1 )) - ZH  l + l - bb (CDF(1.0fb -1 )/D  (1.1fb -1 )) - ZH  bb (CDF(1.7fb -1 )/D  (2.1fb -1 )) - ZH  bb (CDF(1.7fb -1 )/D  (2.1fb -1 )) > H   (From CDF !) > H   (From CDF !) - Simultaneous Search for - Simultaneous Search for WH/ZH/VBF/ggH   +2jets WH/ZH/VBF/ggH   +2jets iii. Combined Results iv. Conclusions iggs (Luminosity) Brand New !

3. The Tevatron @ Fermilab March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p3/18 2KM  pp collisions at 1.96 TeV  36x36 @ 396 ns bunch crossing  ~3.0 fb –1 data on tape.  Initial instantaneous luminosity Record: 2.9 x10 32 cm –2 s –1 Record: 2.9 x10 32 cm –2 s –1  6~8 fb –1 expected by end of 2009 CDF In this talk

4. CDF/D ø Detectors March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p4/18  Multipurpose detectors : “Classic onion-like design” “Classic onion-like design” - Trackers inside solenoid - Trackers inside solenoid - Calorimeters(EM/Had) - Calorimeters(EM/Had) - Muon chambers - Muon chambers  Both running well ! Broad physics programs are actively ongoing !

5. SM Higgs Boson  The Standard Model has been well tested against experimental data and so far provided against experimental data and so far provided great success in particle physics. great success in particle physics. - BUT one particle undiscovered yet. - BUT one particle undiscovered yet. -> “Higgs Boson” : -> “Higgs Boson” : - “Origin of Mass” for all fermions & W/Z bosons. - “Origin of Mass” for all fermions & W/Z bosons. - “Origin of Electroweak symmetry breaking”. - “Origin of Electroweak symmetry breaking”. - Spin 0, Charge 0 - Spin 0, Charge 0  Why so difficult to find Higgs ? - Small production cross section. - Small production cross section. - Large backgrounds. - Large backgrounds. - The SM (by itself) does not predict the value - The SM (by itself) does not predict the value of the Higgs boson mass directly. of the Higgs boson mass directly. (possible through radiative corrections though) (possible through radiative corrections though)  Challenging but the most important task in High Energy Physics. in High Energy Physics. March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p5/18

6. Low Mass Preferred ! March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p6/18 With 2007 Tevatron Combined M top = 170.9 ± 1.8 GeV/c 2  Direct search @ LEP excludes M H <114.4 GeV @ 95% C.L.  SM global fit gives the first indication on where to look !  The most probable value from SM global fit : 76  GeV Upper bound (95% C.L) : <144 GeV (182 GeV if LEP limit included) Upper bound (95% C.L) : <144 GeV (182 GeV if LEP limit included) 33 24

7. Production & Decay @ Tevatron March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p7/18 Production (pp @ 1.96 TeV) Higgs Decay  Main Channels @ Tevatron : - WH  lvbb - WH  lvbb - ZH  vvbb - ZH  vvbb - ZH  llbb - ZH  llbb * H  : New results from CDF ! M H (GeV) 95%CL(LEP) 95%CL(SM fit)  This talk focuses on low mass region. (M H <~140 GeV) (M H <~140 GeV)  High mass search will be presented by next speaker (L. Zivkovic). next speaker (L. Zivkovic). Next Talk

8. WH  lvbb March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p8/18  Lepton P T & Met > 20 GeV  2jets with 1 or 2 b-tagged.  Main backgrounds are W+bb, QCD, ttbar. W+bb, QCD, ttbar.  Employ Neural Net Technique to separate signal from bkg. to separate signal from bkg. Bjet tagging Dijet Mass (1bjet event) Dijet Mass (2bjet events) CDF updates:  Added 1 b events with NN flavor with NN flavor separation. separation.  Included forward electrons. electrons. * See T. Masubuchi’s talk in YSF. talk in YSF.

9. WH  lvbb (cont.) March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p9/18 No significant excess in signal region both in CDF/D . -> Set limits for exclusion! 2bjet 1bjet 2bjet 1bjet NN Configuration: Signal  1 Background  0

10. Limit on WH  lvbb March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p10/18  95% Confidence Level Upper limit is set by binned likelihood method. -> Showing  (limit)/  (SM) Ratio (i.e. If reached 1, it is excluded) -> Showing  (limit)/  (SM) Ratio (i.e. If reached 1, it is excluded)  CDF: (at M H =115 GeV)  (limit)/  (SM) = 8.2/7.3 (obs./exp.)  (limit)/  (SM) = 8.2/7.3 (obs./exp.)  D  : (at M H =115 GeV)  (limit)/  (SM) = 11/9 (obs./exp.)  (limit)/  (SM) = 11/9 (obs./exp.)

11. ZH  llbb (1fb -1 results) March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p11/18  2 high P T leptons from Z -> Clean signature ! -> Clean signature !  Improve dijet mass resolution with Met resolution with Met projection. projection.  Optimized by NN. 95% CL Limit (relative to SM) CDF: 16/16 (obs./expected) D  : 18/20 (obs./expected) at M H =115 GeV Dijet Mass *Summer 2007 results

12. ZH  vvbb (Met+bb) March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p12/18 v v  Met > 50 GeV  Require 2 b jets  QCD estimate/reduction: CDF: NN with Track based Met CDF: NN with Track based Met D  : Asymmetry between D  : Asymmetry between Met and SumEt etc. Met and SumEt etc.  New D  result: Boosted Decision Tree Method. Recovered WH  lvbb D  New CDF Data driven

13. Limit on Met+bb Channel March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p13/18  CDF: (at M H =115 GeV)  (limit)/  (SM) = 8/8.3 (obs./exp.)  (limit)/  (SM) = 8/8.3 (obs./exp.)  D  : (at M H =115 GeV)  (limit)/  (SM) = 7.5/8.4 (obs./exp.)  (limit)/  (SM) = 7.5/8.4 (obs./exp.) *See YSF talk by C. Ochando ! New

14. WH/ZH/VBF/ggH   + 2jets March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p14/18  H   is hard due to small BR (10% of bb).  But we should not give up ! Ideas are : 1. Recover BR by looking at W/Z->2jets: 1. Recover BR by looking at W/Z->2jets: - W  lv(22%), Z  ll(6%), Z  vv(20%) - W  lv(22%), Z  ll(6%), Z  vv(20%) - W  jj (67%), Z  jj(70%) - W  jj (67%), Z  jj(70%) 2. Add all possible channels: 2. Add all possible channels: - Simultaneous search for WH+ZH+VBF+ggH - Simultaneous search for WH+ZH+VBF+ggH 3. Many good kinematic variables to separate 3. Many good kinematic variables to separate signal from backgrounds (dijet mass, d  (j,j) etc). signal from backgrounds (dijet mass, d  (j,j) etc). Brand New

15. NEW Result: H   Channel March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p15/18 * Established background estimate & modeling. * Further improvement by adding 0j/1jet events. * Becomes more interesting at LHC.  Use  lep  had mode. - Lepton P T > 10 GeV - Lepton P T > 10 GeV - Hadronic  P T > 15 GeV - Hadronic  P T > 15 GeV  3 Neural Nets are trained: Signal vs Z->  + jets Signal vs Z->  + jets Signal vs ttbar Signal vs ttbar Signal vs QCD Signal vs QCD  Then select Minimum of 3 NN scores to fit the data. to fit the data. Brand New  CDF: (at M H =120 GeV)  (limit)/  (SM) = 30/24 (obs./exp.)  (limit)/  (SM) = 30/24 (obs./exp.)

16. Combined Results March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p16/18 Combined CombinedCDF DDDD WH  lvbb 1.7 fb -1 (old !) 1.7 fb -1 ZH  llbb 1.0 fb -1 1.1 fb -1 ZH  vvbb 1.7 fb -1 0.93 fb -1 (old !)  Work still in progress to combine all updated & new analyses. all updated & new analyses.  Corresponding luminosity for each analysis used in each analysis used in combination in this talk. combination in this talk. High mass search will be shown in next talk !  Systematic uncertainties are treated as nuisance parameters with truncated as nuisance parameters with truncated Gaussian constraint. After combined, Gaussian constraint. After combined, If significant excess found  Do more checks. If significant excess found  Do more checks. If no excess  Set 95% C.L. Limit. If no excess  Set 95% C.L. Limit.  At M H =115 GeV, Observed Limit (  (limit)/  (SM) ) is 6.2 while expected is 4.3 ! We are getting close to exclude if No Higgs around this region ! We are getting close to exclude if No Higgs around this region ! http://arxiv.org/abs/0712.2383

17. Summary & Prospects March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p17/18  New results with ~2.0 fb -1 data. - We have +1.0 fb -1 already on tape. - We have +1.0 fb -1 already on tape. - New analysis (H   ) done. - New analysis (H   ) done.  In low mass range, the exclusion limit is ~ x 5 to SM prediction, and limit is ~ x 5 to SM prediction, and improving beyond luminosity scaling. improving beyond luminosity scaling.  Advanced technique and better  Advanced technique and better understanding of data etc. understanding of data etc.  Further improvements actively in progress in CDF/D  : in progress in CDF/D  : - Extending lepton coverage. - Extending lepton coverage. - Improving btagging quality etc. - Improving btagging quality etc.  More results coming soon !  Details on each analysis and combined results: - CDF : http://www-cdf.fnal.gov/physics/new/hdg/hdg.html - CDF : http://www-cdf.fnal.gov/physics/new/hdg/hdg.html - D  : http://www-d0.fnal.gov/Run2Physics/WWW/results/higgs.htm - D  : http://www-d0.fnal.gov/Run2Physics/WWW/results/higgs.htm

18. ConclusionConclusion March 2 nd 2008 :: Low Mass Higgs Search :: Kohei Yorita (U. of Chicago) :: p18/18 Yes, “Spontaneous Symmetry Breaking” might be seen at Tevatron ! Or if nature doesn’t like SM Higgs, we need to exclude it a.s.a.p. ! In both cases, it is still a great time to search for SM Higgs at Tevatron.

19. BackupBackup

20. Ref.) CDF SECVTX btag Mistag rate Tagging efficiency

21. More Plots : Met+2jets

22. More Plots : H   Channel Lep+Met+Tau Mass Delta  (j1,j2) Dijet Mass

23. More Plots : H   Channel > 3 Neural Nets Distributions:

24. Further Combination > Results we already have now, but not used in current combination: current combination: 1. WH -> lvbb(CDF): 1. WH -> lvbb(CDF): +200pb -1, 1tag improvement, forward electron inclusion. +200pb -1, 1tag improvement, forward electron inclusion. 2. ZH -> vvbb(CDF): 2. ZH -> vvbb(CDF): Data driven QCD estimate. Data driven QCD estimate. 3. ZH -> vvbb(D  ): 3. ZH -> vvbb(D  ): +1200pb -1 with Boosted Decision Tree Technique. +1200pb -1 with Boosted Decision Tree Technique. 4. H ->  (CDF): 4. H ->  (CDF): New analysis with 2.0fb -1. New analysis with 2.0fb -1. - All combined results coming very soon ! - All combined results coming very soon ! > Other analysis updates (e.g. ZH->llbb) are also ongoing and will be done shortly. ongoing and will be done shortly.