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The Higgs Boson & Beyond To Higgs or not to Higgs? just one of the questions being studied at the LHC John Ellis King’s College London (& CERN)

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Presentation on theme: "The Higgs Boson & Beyond To Higgs or not to Higgs? just one of the questions being studied at the LHC John Ellis King’s College London (& CERN)"— Presentation transcript:

1 The Higgs Boson & Beyond To Higgs or not to Higgs? just one of the questions being studied at the LHC John Ellis King’s College London (& CERN)

2 Open Questions beyond the Standard Model What is the origin of particle masses? due to a Higgs boson? Why so many types of matter particles? What is the dark matter in the Universe? Unification of fundamental forces? Quantum theory of gravity? LHC

3 Some Questions What is it? –Higgs or …? What else is there? –Supersymmetry or …? What next? –A Higgs factory or …?

4 The Seminal Papers The only one who mentioned a massive scalar boson

5 A Phenomenological Profile of the Higgs Boson First attempt at systematic survey

6 A Preview of the Higgs Boson @ LEP First LEP Yellow Report in 1976: – Higgsstrahlung “Bjorken process”

7 A Preview of the Higgs Boson @ LHC Prepared for LHC Lausanne workshop 1984

8 First attempts in 1990, Easier after the discovery of the top quark Estimating the Mass of the Higgs Boson JE, Fogli & Lisi 1991

9 Calculating the Mass of the Higgs Boson Expensive – but maybe not my most costly calculation …

10 2011: Combining Information from Previous Direct Searches and Indirect Data m H = 125 ± 10 GeV Gfitter collaboration

11 Higgs Production at the LHC A la recherche du Higgs perdu … Many production modes measurable if M h ~ 125 GeV

12 Couplings proportional to masses (?) Important couplings through loops: –gluon + gluon → Higgs → γγ Higgs Decay Branching Ratios Many decay modes measurable if M h ~ 125 GeV

13 Higgsdependence Day!

14 Unofficial Combination of Higgs Search Data from December 13th Is this the Higgs Boson? No Higgs here! No Higgs here!

15 The Particle Higgsaw Puzzle Is LHC finding the missing piece? Is it the right shape? Is it the right size?

16 What is it ? Does it have spin 0 or 2? Is it scalar or pseudoscalar? Is it elementary or composite? Does it couple to particle masses? Quantum (loop) corrections? What are its self-couplings?

17 What is the Spin of the ‘Higgs’? Decays into γγ, so cannot have spin 1 Spin 0 or 2? Selections of WW and ZZ events are based on spin 0 hypothesis Can diagnose spin via –angular distribution of γγ –angular correlations of leptons in WW, ZZ decays –Production in association with W or Z

18 Does the ‘Higgs’ have Spin Two ? Vector boson + ‘Higgs’ combined invariant mass very different for spins 0 and 2 JE, Hwang. Sanz & You: arXiv:1208.6002

19 Would have graviton-like couplings: Coefficients somewhat model-dependent Warped compactification: Expect equal couplings for photons, gluons Larger coefficients for W, Z, b, t Smaller coefficients for u, d, s, c (Also expect vector mass < tensor mass X LHC) Does the ‘Higgs’ have Spin Two ? JE, Sanz & You, arXiv:1211.3068

20 Fit of vector-boson couplings to spin-two model Prediction of AdS-type graviton-like model disfavoured by > 3 σ Does the ‘Higgs’ have Spin Two ? JE, Sanz & You, arXiv:1211.3068

21 Does the ‘Higgs’ have Spin Two ? Discriminate spin 2 vs spin 0 via angular distribution of decays into γγ JE, Fok, Hwang, Sanz & You: arXiv:1210.5229 JE & Hwang: arXiv:1202.6660 Monte Carlo simulations

22 The ‘Higgs’ probably does not have Spin Two ATLAS γγ analysis prefers spin 0 over 2 + No discrimination from CMS ZZ* analysis 2 + disfavoured @ 91%

23 What is it ? Does it have spin 0 or 2? –Spin 2 seems unlikely, but needs experimental checks Is it scalar or pseudoscalar? Is it elementary or composite? Does it couple to particle masses? Quantum (loop) corrections? What are its self-couplings?

24 Kinematic distribution of ZZ* final state 0 - disfavoured @ 97% level The ‘Higgs’ probably has Parity +

25 What is it ? Does it have spin 0 or 2? –Spin 2 seems unlikely, but needs experimental checks Is it scalar or pseudoscalar? –Pseudoscalar disfavoured by experiment Is it elementary or composite? Does it couple to particle masses? Quantum (loop) corrections? What are its self-couplings?

26 Elementary Higgs or Composite? Higgs field: ≠ 0 Quantum loop problems Fermion-antifermion condensate Just like QCD, BCS superconductivity Top-antitop condensate? needed m t > 200 GeV New technicolour force? -Heavy scalar resonance? -Inconsistent with precision electroweak data? Cut-off Λ ~ 1 TeV with Supersymmetry? Cutoff Λ = 10 TeV

27 Higgs as a Pseudo-Goldstone Boson Loop cancellation mechanism SupersymmetryLittle Higgs ‘Little Higgs’ models (breakdown of larger symmetry)

28 General Analysis of ‘unHiggs’ Models Parametrization of effective Lagrangian: Fits Azatov, Contino, Galloway: arXiv:1202.3415 a ≠ c CMS fit assuming c > 0 c a

29 Global Analysis of Higgs-like Models Rescale couplings: to bosons by a, to fermions by c Standard Model: a = c = 1 JE & Tevong You, arXiv:1207.1693 JE & Tevong You, arXiv:1204.0464 CDF/D 0 ATLASCMS Update from Kyoto Global

30 What is it ? Does it have spin 0 or 2? –Spin 2 seems unlikely, but needs experimental checks Is it scalar or pseudoscalar? –Pseudoscalar disfavoured by experiment Is it elementary or composite? –No significant deviations from Standard Model Does it couple to particle masses? Quantum (loop) corrections? What are its self-couplings?

31 It Walks and Quacks like a Higgs Do couplings scale ~ mass? With scale = v? Standard Model Higgs: ε = 0, M = v Global fit Update from Kyoto JE & Tevong You, arXiv:1207.1693

32 It Walks and Quacks like a Higgs Do couplings scale ~ mass? With scale = v? Red line = SM, dashed line = best fit JE & Tevong You, arXiv:1207.1693 Global fit Update from Kyoto

33 What is it ? Does it have spin 0 or 2? –Spin 2 seems unlikely, but needs experimental checks Is it scalar or pseudoscalar? –Pseudoscalar disfavoured by experiment Is it elementary or composite? –No significant deviations from Standard Model Does it couple to particle masses? –Some prima facie evidence that it does Quantum (loop) corrections? What are its self-couplings?

34 Loop Corrections ? Experimental limits on anomaly coefficients Anomalous triangle diagrams > Standard Model? Global fit JE, Sanz & You, arXiv:1211.3068

35 What is it ? Does it have spin 0 or 2? –Spin 2 seems unlikely, but needs experimental checks Is it scalar or pseudoscalar? –Pseudoscalar disfavoured by experiment Is it elementary or composite? –No significant deviations from Standard Model Does it couple to particle masses? –Some prima facie evidence that it does Quantum (loop) corrections? –γγ coupling > Standard Model? What are its self-couplings?

36 What is it ? Does it have spin 0 or 2? –Spin 2 seems unlikely, but needs experimental checks Is it scalar or pseudoscalar? –Pseudoscalar disfavoured by experiment Is it elementary or composite? –No significant deviations from Standard Model Does it couple to particle masses? –Some prima facie evidence that it does Quantum (loop) corrections? –γγ coupling > Standard Model? What are its self-couplings? Wait for HL-LHC …?

37 Theoretical Constraints on Higgs Mass Large M h → large self-coupling → blow up at low-energy scale Λ due to renormalization Small: renormalization due to t quark drives quartic coupling < 0 at some scale Λ → vacuum unstable Vacuum could be stabilized by Supersymmetry Degrassi, Di Vita, Elias-Miro, Giudice, Isodori & Strumia, arXiv:1205.6497

38 Vacuum Instability in the Standard Model Very sensitive to m t as well as M H Present vacuum probably metastable with lifetime >> age of the Universe Degrassi, Di Vita, Elias-Miro, Giudice, Isodori & Strumia, arXiv:1205.6497

39 What else is there? Supersymmetry

40 Data Electroweak precision observables Flavour physics observables g μ - 2 Higgs mass Dark matter LHC MasterCode: O.Buchmueller, JE et al.

41 Search with ~ 5/fb @ 8 TeV Jets + missing energy

42 O. Buchmueller, R. Cavanaugh, M. Citron, A. De Roeck, M.J. Dolan, J.E., H. Flacher, S. Heinemeyer, G. Isidori, J. Marrouche, D. Martinez Santos, S. Nakach, K.A. Olive, S. Rogerson, F.J. Ronga, K.J. de Vries, G. Weiglein

43 LHCb finds ~ (1 ± 0.3) × Standard Model Measurements of B s  μ + μ - Update from Kyoto

44 5 --- 1/fb ___ 5/fb p-value of simple models < 10% 1 Buchmueller, JE et al: arXiv:1207.3715 With LHCb update from Kyoto CMSSM

45 5 1 Favoured values of gluino mass significantly above pre-LHC, > 1.5 TeV Gluino mass Buchmueller, JE et al: arXiv:1207.3715 CMSSM With LHCb update from Kyoto

46 5 1 Favoured values of close to Standard Model: Almost no change with new LHCb result Bs μ+μ-Bs μ+μ- Buchmueller, JE et al: arXiv:1207.3715 CMSSM With LHCb update from Kyoto

47 X ENON 100 & other Experiments

48 Favoured values of dark matter scattering cross section significantly below XENON100 5 --- 1/fb ___ 5/fb Buchmueller, JE et al: arXiv:1207.3715 Spin-independent Dark matter scattering Excluded by XENON100 Excluded by LHC 2

49 Favoured regions of parameter space Focus on the coannihilation strip Small mass difference – long-lived stau? What remains for the CMSSM? Citron, JE, Luo, Marrouche, Olive, de Vries: arXiv:1212.2886

50 Stau lifetime sensitive to Δm, may be long May decay inside or outside the detector Decays into 1 or 3 charged particles, also neutrals What remains for the CMSSM? Citron, JE, Luo, Marrouche, Olive, de Vries: arXiv:1212.2886

51 Small Δm favoured in χ 2 analysis May decay inside or outside the detector Search for long-lived Staus? Citron, JE, Luo, Marrouche, Olive, de Vries: arXiv:1212.2886

52 Conversation with Mrs Thatcher: 1982 What do you do? Think of things for the experiments to look for, and hope they find something different Wouldn’t it be better if they found what you predicted? Then we would not learn anything!

53 The ‘Higgs Legacy’? Seize the moment to engage students, general public, Government, …. –Local communities –Schools –Visits to CERN –Science centres –MPs ‘Higgs Day’ Nov. 7 th 2013?

54 What Next: A Higgs Factory? To study the ‘Higgs’ in detail: The LHC –Rethink LHC upgrades in this perspective? A linear collider? –ILC up to 500 GeV –CLIC up to 3 TeV (Larger cross section at higher energies) A circular e+e- collider: LEP3, … –A photon-photon collider: SAPPHiRE A muon collider

55 e + e - Collider Summary ICFA Higgs Factory Workshop Fermilab, Nov. 2012


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