Higgs Searches at the Tevatron Run I Lorenzo

  • Slides: 20
Download presentation
Higgs Searches at the Tevatron (Run I) Lorenzo Moneta University of Geneva on behalf

Higgs Searches at the Tevatron (Run I) Lorenzo Moneta University of Geneva on behalf of CDF and D collaboration • Introduction • SM Higgs ¯ (CDF & D ) – ZH & WH with H bb • MSSM Higgs ¯ with f=H 0, h 0, A 0 (CDF) – bbf – H+ (CDF & D ) • Fermiophobic Higgs – H gg (CDF & D ) • Conclusions Lorenzo Moneta Moriond QCD 17 -23 March 2001 1

Introduction • Electroweak Symmetry breaking in the SM predicts existence of an Higgs boson

Introduction • Electroweak Symmetry breaking in the SM predicts existence of an Higgs boson but with unspecified mass – Higgs mass constraints scale where SM might break down • if = MPlank then 130 < M(H) < 180 Current Status of Higgs searches • SM fit to Electroweak data indicates a light Higgs – M(H) < ~ 200 Ge. V @ 95 % CL • Direct searches from LEP 2 – 95 % CL limit is ~ 113 Ge. V – Indication of Higgs-like events in the last year data: excess ~ 3 at M(H) 115 Ge. V Lorenzo Moneta Moriond QCD 17 -23 March 2001 2

Tevatron (Run I) Tevatron proton-antiproton collision @ s = 1. 8 Te. V CDF

Tevatron (Run I) Tevatron proton-antiproton collision @ s = 1. 8 Te. V CDF DØ Run I (Oct. 92 Feb. 96) Silicon Vertex Detector total integrated luminosity ~ 120 -1 pb / detector Expected ~ 2 fb-1 in Run IIa ! Lorenzo Moneta Moriond QCD 17 -23 March 2001 3

SM H 0 production @ Tevatron • Gluon Fusion = 0. 70 pb for

SM H 0 production @ Tevatron • Gluon Fusion = 0. 70 pb for M(H) = 120 Gev/c 2 with QCD NLO correction – too difficult (QCD background) • Higgsstrahlung WH: = 0. 16 pb ZH: = 0. 10 pb – SM cross section is very small • 1/20 (t-tbar) • 1/500 (Z/W + 2 jets) – possible with Run II luminosity ! – larger with new physics ? ? Lorenzo Moneta LEP • • Vector Boson fusion radiation off heavy quark Moriond QCD 17 -23 March 2001 • very small in the SM 4

SM Higgs decays • M(H) < 130 Ge. V – dominant decay is –

SM Higgs decays • M(H) < 130 Ge. V – dominant decay is – final states are for W/ZH – need lepton ID/MET + b-tags • M(H) > 130 Ge. V – dominant decay is – final state with 2 leptons LEP For M(H) = 120 Ge. V/c 2 – but smaller cross-section • interesting at Run. II ! Lorenzo Moneta Moriond QCD 17 -23 March 2001 5

SM H signatures (W /Z + H) Tevatron Run I channels : (W/Z +

SM H signatures (W /Z + H) Tevatron Run I channels : (W/Z + H with M(H) < 130 Ge. V) • ( 50% of W/Z H ) – BG: QCD multijets • ( 9% ) – BG: • ( 5. 4%) – BG: QCD, • ( 1. 8%) – BG: Lorenzo Moneta Essential for these analyses: • b tagging • good di-jet mass resolution Moriond QCD 17 -23 March 2001 6

b tagging at the Tevatron Techniques developed for top analyses. Two algorithms: – Soft

b tagging at the Tevatron Techniques developed for top analyses. Two algorithms: – Soft Lepton Tagging (SLT) (CDF & DØ) • semileptonic b decays: b • DØ: m ( p. T > 4 Ge. V) CDF: m & e (p. T > 2 Ge. V) e, µ (in jets) e(b-tag) ~ 7%/b-jet e(mistag) ~ 0. 5%/jet – Secondary Vertex Tagging (SVX) (CDF) • reconstruct a displaced vertex in the jet • b lifetime ~ 1. 5 ps decay length ~ few mm • use capability of Silicon vertex detectors (decay-length) ~ 100 mm b jet primary vertex Lorenzo Moneta secondary vertex Moriond QCD 17 -23 March 2001 e(b-tag) ~ 20%/b-jet e(mistag) ~ 0. 2%/jet 7

Search for • Final states are lepton (e/m) + MET + b’s • Event

Search for • Final states are lepton (e/m) + MET + b’s • Event selection: – – CDF high p. Tlepton: p. T(lep) > 20 Ge. V & <1 MET>20 2 jets with ET(j)>15, <2 b-tags (single OR double jet tag) 1 b-tag • Backgrounds: 2 b-tags – Results (CDF & D ) 106 pb-1 Exp. channel backg data Br x accept. (90<m(H)<130) CDF 1 b-tag 30 5 36 ~ 0. 6 – 0. 8 % CDF 2 b-tags 3 1 6 ~ 0. 2 – 0. 3 % D 1 b-tag 25 3 27 ~ 0. 6 - 0. 9 % Lorenzo Moneta mbb from fit to di-jets mass: 95% CL Limit on BR: 26 -28 pb for 90<MH<130 (CDF) 40 -19 pb for 90<MH<120 (D ) Moriond QCD 17 -23 March 2001 8

Search for • Final states is MET + b’s • Event selection (CDF): –

Search for • Final states is MET + b’s • Event selection (CDF): – MET>40 (trigger >35) + lepton veto – 2 or 3 jets with ET(j)>15, <2 – DF(MET, j) > 60° for all jets (ET>8) – DF(j 1, j 2) < 150° – b-tags (single OR double) • Backgrounds: – QCD and Results (88 pb-1) Exp. channel backg data Br x accept. (90<m(H)<130) CDF 1 b-tag 39 4 40 ~ 0. 5 – 0. 8 % CDF 2 b-tags 4 1 4 ~ 0. 4 – 0. 5 % Lorenzo Moneta Moriond QCD 17 -23 March 2001 95% CL Limit on BR: ~ 8 pb for 90<MH<130 9

Search for • Final states is di-leptons + b’s • Event selection (CDF): –

Search for • Final states is di-leptons + b’s • Event selection (CDF): – p. T(lep)>20, 10 Ge. V – 76<M(l, l)<106 Ge. V – 2 or 3 jets with ET(j)>15, <2 – MET < 50 Ge. V (against top di-lepton evts) – 1 b-tag • Backgrounds: – Results (106 pb-1) Exp. channel backg data Br x accept. (90<m(H)<130) CDF 1 b-tag 3 1 5 ~ 0. 2 % Lorenzo Moneta Moriond QCD 17 -23 March 2001 mbb 95% CL Limit on BR: 56 -24 pb for 90<MH<130 10

Search for • Multi-jet final state with b’s • Event selection (CDF): – Multi-jets

Search for • Multi-jet final state with b’s • Event selection (CDF): – Multi-jets trigger • 4 jets with SET>125 Ge. V & ET>15 – double b-tag ¯ – p. T(bb)>50 Ge. V • Backgrounds: – mainly QCD (b’s + fakes) – also top and Z + jets Results (91 pb-1) Exp. channel back. data Br x accept. (90<m(H)<130) CDF 2 b-tag ~ 600 589 ~ 1. 5 – 2. 9 % Need good Mbb resolution against background Lorenzo Moneta Moriond QCD 17 -23 March 2001 mbb 95% CL Limit on BR: 30 -16 pb for 90<MH<130 11

Combined limit for SM Higgs CDF combination of 95 % CL limit on limit

Combined limit for SM Higgs CDF combination of 95 % CL limit on limit = 7. 4 -8. 2 pb for m. H = 90 -130 Ge. V/c 2 • x 30 SM cross-section (m. H = 115) LEP SM 115 Lorenzo Moneta ¯ • Limit is dominated by nnbb • Expected best limits from: – ¯ and lnbb ¯ nnbb ¯ limit due to a small • poor lnbb excess in observed events • Need more luminosity – RUN II Moriond QCD 17 -23 March 2001 12

MSSM Higgs Search Two Higgs doublets in the MSSM – 5 Higgs particles •

MSSM Higgs Search Two Higgs doublets in the MSSM – 5 Higgs particles • two neutral CP-even: h 0, H 0 • One neutral CP odd: A 0 • Two charged: H+, H- – two free parameters: tanb and m. A – Mass relations at tree level: • m(h 0) < m(Z 0) < m(H 0); m (A 0) < m(H 0); m(H+) < m(W) • but after radiative corrections m(h 0) < 130 Ge. V – Couplings at large tanb: • enhanced to d-type quark and leptons • suppressed to u-type quark Lorenzo Moneta Moriond QCD 17 -23 March 2001 13

MSSM Higgs production h h H H tanb = 30 (pb) tanb = 3

MSSM Higgs production h h H H tanb = 30 (pb) tanb = 3 • Small tanb : • Large tanb – SM-like cross-sections ¯ coupling – enhanced hbb ¯ ¯ ¯ can have large – hbb/Hbb/Abb cross-sections ( tan 2 b) ¯ (90%) and t+t- (10%) In general dominant Higgs’s Branching Ratio are to bb Lorenzo Moneta Moriond QCD 17 -23 March 2001 14

Search for ¯ production ( • Exploit enhanced Yukawa couplings looking for bb =

Search for ¯ production ( • Exploit enhanced Yukawa couplings looking for bb = h, HA) • large cross sections ( tanb 2) • 4 -b’s jets final state • Event selection (CDF): – Multi-jets trigger • 4 jets with S(ET)>125 Ge. V & ET>15 – ET(j) cuts depending on m( ) – 3 b-tags ¯ > 109° (against g bb) – DF(bb) • Backgrounds: – ¯ QCD (bb/cc), Z/Wjj, top Lorenzo Moneta CDF results (91 pb-1) M( ) (Ge. V) 70 BR x acc. backg data 0. 16 % 4. 6 1. 4 5 120 0. 28 % 3. 5 1. 1 2 300 0. 59 % 0. 1 0. 4 0 Moriond QCD 17 -23 March 2001 15

Limit for • Limit (95%CL for M = 100 Ge. V): BR < 25.

Limit for • Limit (95%CL for M = 100 Ge. V): BR < 25. 7 pb • convert BR limit in tanb vs Higgs mass exclusion – No mixing & Maximal Mixing for the stop tanb vs m(h) tanb vs m(A) Tevatron complements LEP ! Lorenzo Moneta Moriond QCD 17 -23 March 2001 16

Charged Higgs Searches • Searches for t H+b when M(H+) < mt - mb

Charged Higgs Searches • Searches for t H+b when M(H+) < mt - mb • decay t H+b can compete with SM decay t W+b • BR(t H+b) depends on tanb Direct Search (CDF): • look for H+ tn in t-tbar evts – BR(H+ tn) 1 for large tanb – WHbb or HHbb channels in addition to WWbb – look for l + t + MET + jj events (l = e, m, t) – use t identifications via hadronic decays (tracking + calorimeter) – backgrounds: • Z tt + jj, W+ 3 jets, WW/WZ – acceptances for single and double H production Lorenzo Moneta Moriond QCD 17 -23 March 2001 17

Charged Higgs Searches Indirect Search (CDF + D ) • look for lepton disappearance

Charged Higgs Searches Indirect Search (CDF + D ) • look for lepton disappearance in t-tbar events • • suppression of dileptons and lepton + jets events rate of the two depends on BR(t H+b) t-tbar cross-section independent of m(H), tanb given measured x-section (when BR(t H+b) = 0) exclusion regions in the m(H+)-tanb plane D 0 LEP 2 (ADLO) New Exclusion regions at low and high tanb Lorenzo Moneta Moriond QCD 17 -23 March 2001 18

Fermiophobic Higgs • In some models Higgs couples only to vector bosons • BR(H

Fermiophobic Higgs • In some models Higgs couples only to vector bosons • BR(H gg) dominant for light Higgs (m(H) < 100) • Searches for W/Z + H ggjj – D search: • di-photons + jets • Backgrounds from QCD D 0 – fakes or real g in jets – CDF search • di-photons with e/m + MET or jj • Limit For SM cross-section: M(H) > ~ 80 Ge. V (95% CL) • LEP limit is ~ 105 Ge. V Lorenzo Moneta Moriond QCD 17 -23 March 2001 19

Conclusions • SM Higgs searches are luminosity limited in Run I – – no

Conclusions • SM Higgs searches are luminosity limited in Run I – – no sensitivity to SM cross sections no excess seen and set limits at ~30 SM cross-section provided experience for Run II developed techniques for low mass Higgs searches • b tagging and di-jet mass resolution are crucial ! – good expectations for Run II see next talk on Run II prospects report of the Tevatron Higgs Working Group (hep-ph/0010338) • Nice exclusion results for MSSM Higgs: – – bb search with sensitivity for high tanb region charged Higgs from t H+b probed regions inaccessible to LEP very interesting in Run II Lorenzo Moneta Moriond QCD 17 -23 March 2001 20