Higgs Coupling Measurements!

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Status, prospects, and interplay with searches for physics BSM Seminar University of California - Irvine April 23rd, 2014

Introduction Fantastic progress since discovery July 2012 Observation in three boson channels Evidence for fermion couplings Precision mass measurement ~126 GeV Spin determined Looks more and more like the SM Higgs boson arxiv:1312.5353 No evidence for non-sm decays No evidence for additional Higgs bosons ATLAS and CMS are finalizing final Run I papers and are preparing combinations ATLAS-CONF-2013-012 2

Introduction Is there BSM physics hidden in the Higgs sector? Experimental post-discovery approach Measure (126 GeV) Higgs properties Search for additional Higgs bosons Search for BSM in signatures with Higgs bosons Search for BSM Higgs decays 3

Introduction Gateways to BSM physics in the 126 GeV Higgs Mixing Loops Decays In general BSM physics modifies absolute value and tensor structure we factorize the problem, knowing that this is incorrect 4

Higgs coupling measurements 5

Coupling Measurements Strategy: narrow width approximation Measurement: parametrize deviations wrt SM in production and decay implies precise knowledge of the SM prediction BSM acceptance effects are not considered 6

LHC Higgs production and decay mh = 125 GeV, 8 TeV mh = 125 GeV Process Diagram Cross section [fb] Unc. [%] Decay BR [%] Unc. [%] gluon-gluon fusion vector boson fusion 19520 15 1578 3 bb 57.7 3.3 ττ 6.32 5.7 cc 2.91 12.2 WH 697 4 ZH 394 5 tth 130 15 μμ 0.022 6 WW 21.5 4.3 gg 8.57 10.2 ZZ 2.64 4.3 γγ 0.23 5 Zγ 0.15 9 ΓH [MeV] 4.15 4 * uncertainties need improvements for future precision measure 7

Available Channels untagged jet-tag VBF VH tth H γγ used H WW 2l2v H ZZ 4l possible H bb H ττ H Zγ H μμ H invisible simplified view 8

Cross Contamination ATLAS-CONF-2014-009 9

Total Width SM Higgs total width Γ H 4.2 MeV Indirect constrained in coupling fits assuming SM Higgs coupling requires further assumptions Measurements at the LHC interference between Higgs signal and continuum c results in Higgs mass shift off-shell H* production in H* ZZ ( * ) (more later) 10

Probing BSM Simultaneous fit of all couplings with several assumptions on total width Searches for new physics in loops: κ g, κγ, BR BSM Fermion vs vector boson couplings: κ V, κ f Search for asymmetries: λ WZ, λ du, λ lq Overall scaling of signal strength: μ 11

Effective Field Theory Approach Parametrize SM deviation by higher-dimensional operators Allows study of large class of BSM models Allows combination with electroweak precision data Does not account for effects of light particles in loops, but theses can be studied with specific BSM models No results from LHC experiments for now. 12

Experimental Status Current Player Future Player 13

Status of LHC Higgs program Channel ATLAS Lumi [1/fb] CMS Lumi [1/fb] Specialty Inclusive signature σ Obs. (Exp.) mass [GeV] Signal Strength μ Spin/ Parity H ZZ 4l 4.6+20.7 ATLAS-CONF- 2013-012 5.1+19.6 arxiv: 1312.5353 mass, discovery, spin/parity 4 leptons 6.6 (4.4) 6.8 (6.7) 124.3 ±0.6 (stat) ±0.5 (sys) 125.6 ±0.4 (stat) ±0.2 (sys) 1.7+0.5-0.4 0.93+0.29-0.25 H WW 2l2v 4.6+20.7 ATLAS-CONF- 2013-030 4.9+19.5 arxiv: 1312.1129 cross section, coupling 2 leptons, MET 3.8 (3.7) 4.3 (5.8) consistent 125 ± 4 1.01 ± 0.31 0.72+0.20-0.18 H γγ 4.8+20.7 ATLAS-CONF- 2013-012 5.1+19.6 CMS-PAS- HIG-13-001 mass, discovery, couplings two photons 7.4 (4.3) 3.2 (4.2) 126.8 ±0.2 (stat) ±0.7 (sys) 125.4 ±0.5 (stat) ±0.6 (sys) 1.65+0.33-0.28 0.78+0.28-0.26 H bb 4.7+20.3 ATLAS-CONF- 2013-079 5.0+18.9 arxiv: 1310.3687 total width, coupling to fermions two b-jets - 2.1 (2.1) consistent consistent 0.2 ± 0.7 1.0 ± 0.5 - - H ττ 20.3 ATLAS-CONF- 2013-108 4.9+19.4 arxiv: 1401.5041 couplings to leptons hadronic taus, leptons, MET 4.1 (3.2) 3.4 (3.6) - 122 ± 7 1.4 + 0.5-0.4 0.78 ± 0.27 - - 14

Tevatron p-value 3.0σ (1.9σ expected) at mh = 125 GeV Measurement of competitive with LHC 15

Progress on tth Direct study of top Yukawa coupling CMS exploring all accessible Higgs decay modes Full program on tth underway in ATLAS Approaching SM sensitivity in 8 TeV data CMS-HIG-13-020 ATLAS-CONF-2014-011 16

Coupling Results CMS coupling fits (HIG-13-005) based on preliminary results released Moriond 13. Updated analyses are available. ATLAS coupling fits (ATLAS-CONF-2014-009) based on preliminary results released Moriond 14 Tevatron results published in Phys.Rev.D88,052014 17

Summary of Signal Strength 18

Vector and fermion coupling 19

Fermion Coupling Asymmetry BSM models (e.g. 2HDM) show asymmetries between up and down type or lepton and quark couplings Three parameter fits Measurement of κ b and κτ coupling allows measurement of λ du Measurement of κτ allows a measurement of λ lq Downtype fermion couplings established by ATLAS (~3.6σ) and CMS (~4.0σ) 20

Lepton Quarks Asymmetry BSM models (e.g. 2HDM) show asymmetries between up and down type or lepton and quark couplings Three parameter fits Measurement of κ b and κτ coupling allows measurement of λ du Measurement of κτ allows a measurement of λ lq Downtype fermion couplings established by ATLAS (~3.6σ) and CMS (~4.0σ) 21

Probing BSM in Loops Effective couplings to gluons and photons 22

Probing BSM in Loops Constrain total width assuming SM Higgs treelevel couplings Degeneracy of BR BSM with gluon coupling from σ(gg H) Direct search for invisible Higgs decays or total width measurements not included 23

Invisible Higgs Decays Direct search for invisible Higgs decays VBF and ZH production modes used so far Gluon fusion production accessible DM interpretation complementary to direct searches arxiv:1404.1344 24

Generic Fits 25

Generic Fits 26

Rare SM Decay Channels Phys.Lett.B732 (2014) Phys.Lett.B726 (2013) Rare SM decay channels can be added to the general coupling fit No direct effect on other couplings, but other channel constrain production modes CMS-HIG-14-003 27

Rare SM Decay Channels BR SM (H μμ)= 2.2 x 10-4 Good resolution, signal tiny, huge background Testing 2nd generation Higgs coupling CMS-HIG-13-007 ATLAS-CONF-2013-010 28

Total Width Measurement Enhancement of cross section at high mass due to Higgs. ~8% in ZZ final state Used to constrain ΓH N. Kauer, G. Passarino, JHEP 08 (2012) 116 F. Koala, K. Melnikov, Phys. Rev. D88 (2013), 054024 J. Cambell et al, arxiv:1311.3589 29

Total Width Measurement Experimental constraint on Higgs total width using H* ZZ Combination of 4l and 2l2v final states Results: r < 4.2 (8.5 expected) @ 95% CL ΓH < 17 MeV (35 MeV expected) @ 95% CL CMS-HIG-14-002 30

Prospects at the HL-LHC and beyond 8 TeV LS1 13-14 TeV LS2 LS3 HL-LHC 2012 2013 2014 2015 2016 2017 2018 2019 2020 2021 2022 2023 2024 0.7x10 34 cm -2 s -1 1x10 34 cm -2 s -1 2x10 34 cm -2 s -1 5x10 34 cm -2 s -1 31

General Coupling Fits κg, κγ, κzγ: loop diagrams allow potential new physics κw, κz: vector bosons κt, κb: up- and down-type quarks κτ, κμ: charged leptons total width from sum of partial widths Assumptions on systematic uncertainties Scenario 1: no change Scenario 2: Δ theory / 2, rest 1/ L precision measurements coupling precision 2-10 % factor of ~2 improvement from HL-LHC arxiv:1307.7135 32

Theoretical Uncertainties To test the importance of theoretical uncertainties we show the effect of removing them. Theoretical uncertainties dominated by QCD scale and PDF uncertainties. Uncertainty on BR become relevant at few % precision. arxiv:1310.8361 Δ theory = 0, rest unchanged 33

Comparison of ATLAS and CMS prospects Large differences in fits for coupling strength ATLAS connects Κτ with Κb to overcome H bb mode, but H ττ then becomes overall limitation in constraining total width. from: ATLAS-PHYS-PUB-2013-014 34

Higgs Couplings at Lepton Collider Higgs-strahlung allows decay mode independent measurement performed on OPAL data benchmark for lepton collider studies Couplings model independent extraction of g ZZH from σ ZH in fit to recoil mass spectrum other Higgs couplings extracted from σ ZH x BR measurements and g ZZH total width extracted from combination of initial and final state measurements precision limited by statistics 35

Potential Future Facilities ILC CLIC Future Circular Collider (FCC) 36

Potential Future Facilities ILC from Chip Brock 37

Higgs Couplings at Lepton Collider arxiv:1310.8361 38

Higgs Self Coupling Very challenging search / measurements interference Cross section at NNLO arxiv:1309.6594 Boosted Higgs bosons HL-LHC required to reach SM sensitivity BSM increase in yields can be substantial Ebullient discussion of di-higgs production by theory community Experimentalists very conservative References in backup 39

Channels and Sensitivity Promising final states at the LHC Difficulties in background estimation esp. fake rate or mistag estimates Expected sensitivity Sensitivity enhanced using event shapes ATLAS & CMS are developing a program for HL-LHC di-higgs measurements Lepton collider need very large datasets at high energy or extreme precision g ZH measurements 40

Summary 41

Higgs physics transitioned from searches to precision measurements Conclusion Signatures compatible with SM Higgs Boson Interpretation in numerous BSM model possible Future precision measurements can unveil true nature of this beast Exciting experimental and theoretical research program ahead 42

Resources ATLAS public Higgs physics page CMS public Higgs physics page Tevatron Higgs page ATLAS & CMS Snowmass and ECFA reports Snowmass Higgs group summary report 43

Resources on Di-Higgs incomplete list 44

Comparison of ATLAS and CMS Uncertainty on signal strength Ranges [x,y] are not directly comparable ATLAS [no theory uncertainty, Scenario 1] CMS [Scenario 2, Scenario 1] Overall reasonable agreement, but ATLAS does not include H bb mode CMS outperforms ATLAS H ττ mode Large differences in H Zγ mode due to photon id Markus Klute(MIT) 45

Uncertainty on Signal Strength Assumptions on systematic uncertainties Scenario 1: no change Scenario 2: Δ theory / 2, rest 1/ L Based on parametric simulation Extrapolated from 2011/12 results Markus Klute(MIT) 46

LHC Upgrade Stages Markus Klute(MIT) LHC Reach 10 34 cm -2 s -1 by LS2, double by LS3 and integrate 300fb -1 by 2022 <PU> = 50 HL-LHC Lumi-level 5x 10 34 cm -2 s -1 and integrate 3000fb -1 after L3 <PU> = 140 47

Higgs Couplings at Lepton Collider Higgs-strahlung is main production process HZZ coupling observed at the LHC Vector boson fusion give small contribution at 250 GeV Cross section plateau at 240-280 GeV Reasonable background level Markus Klute(MIT) 48