technidilaton in light of lhc run ii
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Technidilaton in light of LHC-Run II Shinya Matsuzaki (Institute - PowerPoint PPT Presentation

Technidilaton in light of LHC-Run II Shinya Matsuzaki (Institute for Advanced Research & Department of Physics, Nagoya U.) @ Nagoya Univ. 03/05/2014 Current status on 125 GeV Higgs discovered at LHC CMS-PAS-HIG-13-005 ATLAS: PLB726


  1. Technidilaton in light of LHC-Run II Shinya Matsuzaki (Institute for Advanced Research & Department of Physics, Nagoya U.) @ Nagoya Univ. 03/05/2014

  2. Current status on 125 GeV Higgs discovered at LHC CMS-PAS-HIG-13-005 ATLAS: PLB726 (2013) * measured coupling properties consistent w/ the SM Higgs so far * BUT, is it really the SM Higgs? --- origin of mass put in by hand? --- unnatural elementary Higgs?

  3. It could be a composite scalar, Techni-dilaton (TD) Yamawaki et al (1986); Bando et al (1986) * TD : composite scalar: -- predicted in walking technicolor giving dynamical origin of mass by technifermion condensate -- arises as a pNGB for SSB of (approximate) scale symmetry technifermion condensate -- lightness protected by the scale symmetry (naturalness), and hence can be, say, ~ 125 GeV. S.M. and K. Yamawaki (2012) • 125 GeV TD signatures at LHC are consistent with current data Today: comparison is updated

  4. Contents of this talk: 1. Introduction 2. Walking TC and Technidilaton 3. 125 GeV TD signal vs. current LHC data 4. Toward LHC-Run II 5. Summary

  5. 2. Walking technicolor and TD

  6. Yamawaki et al (1986); Bando et al (1986) Walking TC and techni-dilaton :Pseudo IRFP β QCD-like “walking” ~1000TeV “walking” ~ O(4 π Fπ) = O(1TeV) * Techni-dilaton (TD) emerges as (p)NGB for approx. scale symmetry SSB of (approximate) scale sym . α starts “running” (walking) up to mF Nonpert. scale anomaly TD gets massive induced by mF itself

  7. Light techni-dilaton S.M and K.Yamawaki , PRD86 (2012) * One suggestion from holographic formula for TD mass --- TD mass (lowest pole of dilatation current correlator) “conformal limit” 125 GeV TD is realized by a large gluonic effect : G 〜 10 for one- family model w/ Fπ = 123 GeV (c.f. QCD case, G ~ 0.25 ) 125 GeV

  8. TD Lagrangian below m F S.M. and K. Yamawaki, PRD86 (2012) * effective theory below mF walking regime after TF decoupled/integrated out & confinement : governed by TD and other light TC hadrons * Nonlinear realization of scale and ~O(TeV) ~10^3TeV chiral symmetries Nonlinear base χ for scale sym. w/ TD field Φ TD decay constant F Φ Nonlinear base U for chiral sym. w/ TC pion field π

  9. eff. TD Lagrangian i) The scale anomaly-free part: ii) The anomalous part (made invariant by including spurion field “S”): reflecting ETC-induced TF 4-fermi w/ (3- γ m ) β F : TF-loop contribution iii) The scale anomaly part: t0 beta function which correctly reproduces the PCDC relation:

  10. TD couplings to the SM particles * TD couplings to W/Z boson (from L_inv) * TD couplings to γγ and gg (from L_S) β F : TF-loop contribution t0 beta function

  11. TD couplings to the SM particles * TD couplings to W/Z boson (from L_inv) The same form as SM Higgs couplings * TD couplings to γγ and gg (from L_S) except F Φ and betas β F : TF-loop contribution t0 beta function

  12. * TD couplings to SM fermions * in WTC to get realitic masses w/o FCNC concerning 1 st and 2 nd generations 2 Miransky et al (1989); Matsumoto (1989); Appelquist et al (1989) * in Strong ETC to accommodate masses of the 3rd generations (t, b, tau) 1

  13. Thus , the TD couplings to SM particles essentially take the same form as those of the SM Higgs! : Just a simple scaling from the SM Higgs: But, note φ - gg, φ - γγ depending on particle contents of WTC models. β F : TF-loop contribution t0 beta function

  14. To be concerete, we consider one-family model (1FM ) evaluate betas at one-loop level:

  15. 3. 125 GeV TD Signal vs. LHC-Run I Data

  16. * relevant production processes at LHC similar to SM Higgs: ggF , VBF, VH, ttH * relevant decay channels enhanced by extra (for N TC =4) colored BR techni-quark ---------------------------------------- contribution Φ  gg : ~ 75% Φ  bb : ~ 19 % Φ  WW : ~ 3.5% Φ  ττ : ~ 1.1 % Φ  ZZ : ~ 0.4% Φ  γγ : ~ 0.1%

  17. Updated from S.M. and Yamawaki The signal strength fit to PLB719(2013) the LHC-Run I full data ---------------------------------------------------------------- N TC [v EW /F Φ ]best χ^2 min /d.o.f. One-parameter fit ( Fφ ) ---------------------------------------------------------------- 3 0.28 37/17 = 2.2 --------------------------------------------------------------- 4 0.24 19/17 = 1.1 ---------------------------------------------------------------- 5 0.17 33/17 = 1.9 ---------------------------------------------------------------- Compared w/ SM Higgs NTC=3 χ^2/ d.o.f = 17/18 = 1.0 NTC=5 Current LHC has favored TD at almost the same level as NTC=4 SM Higgs! SM Higgs *

  18. The TD signal strengths (μ = σ x BR/SM Higgs) vs. the current data (i) (i) ggF+ttH category CMS TD signal strength ATLAS * one- family model w/ NTC=4, v EW /F φ = 0.24 * Consistent at 1 sigma level (except CMS-diphoton)

  19. The TD signal strengths (μ = σ x BR/SM Higgs) vs the current data (ii) (ii) VBF +VH category ATLAS TD signal strength CMS * Consistent within 2 sigma error * VBF: contamination from ggF by about 30% taken into account, except bb channel (b-tag) * Smaller VBF+VH signal (particularly, bb-channel), compared to the SM Higgs  Conclusive answer needs high statistic LHC-Run II !

  20. 4. Toward LHC Run-II

  21. Determining TD decay constant F Φ Precise estimate is needed for LHC- Run II * Theoretical predictions so far S.M. and Yamawaki (2012) ladder approximation: holographic estimate: More rigorous estimate should be made directly by lattice simulations! --- needs a way of measuring F Φ on lattice It is actually provided by scale-invariant ChPT!

  22. Scale-invariant ChPT (sChPT) -- Determining TD decay constant F Φ and mass M Φ on lattice S.M. and K. Yamawaki, 1311.3784 (2013) * sChPT is formulated so as to reproduce chiral/scale WT identity: hard-breaking term soft- breaking term and PCDC (and PCAC) at the leading O(p^2): Soft-breaking mass

  23. Note the dilaton mass formula as direct consequence of WT (and PCDC): hard-breaking mass (chiral-limit mass) Soft-breaking mass proportional to mf:

  24. * Building-blocks and order-counting rule

  25. * The leading-order O(p^2) chiral and scale-invariant Lagrangian Note: soft-breaking term is uniquely fixed by stabilization of dilaton potential in the presence of current mass mf

  26. * Dilaton mass formula at O(p^2) is reproduced: * Prefactor fairly insensitive to exact value of γ m in walking theory * is Independent of Nf

  27. Holography (large Ntc limit ) (S.M. and K.Yamawaki, 2012) Just a sample value in between Fitting to LHC phenomenology (S.M. and K.Yamawaki, 2012 and this talk)

  28. * Chiral log (pion mass) corrections to dilaton mass at O(p^4) Counterterms:

  29. * Plot of M Φ vs. M π at O(p^4) w/ assuming counterterms =0 @ μ=Λ χ Chiral log corrections get significant as m π  0 --- crucial for chiral-limit TD mass and decay constant!

  30. 5. Summary

  31. * TD is the characteristic light scalar in WTC: the mass can be 125 GeV: the lightness is protected by approximate scale invariance. * The 125 GeV TD in 1FM gives the LHC signal consistent w/ current LHC data. * More precise measurements in VBF+VH categories will tell us whether TD is the LHC Higgs, or not. * Toward LHC-Run II: --- needs rigorous estimate of TD decay constant --- it is doable on lattices via dilaton mass formula. * Smoking gun of WTC: discovering walking TPs & Techni-rhos (Terashi & Kurachi’s talks)

  32. Backup Slides

  33. K. Haba , S.M. and K. Yamawaki , PRD82 (2010); More on holographic estiamtes Holographic TD S.M. and K.Yamawaki, 1209.2017 S.M. and K.Yamawaki, 1209.2017 * Ladder approximation : gluonic dynamics is neglected * Deformation of successful AdS/QCD model (Bottom -up approach) Da Rold and Pomarol (2005); Erlich, Katz, Son and Stephanov (2005) incorporates nonperturbative gluonic effects 0 5d SU(N TF ) L x SU(N TF) R z UV IR QCD WTC

  34. AdS/CFT dictionary: * UV boundary values = sources * IR boundary values: chiral condensate gluon condensate

  35. * AdS/CFT recipe: generating functional classical solutions sources = UV boundary values for bulk scalar, vector, axial-vector fields Current collerators are calculated as a function of three IR –boundary values and : dual : IR value of bulk scalar : IR value of bulk scalar : IR-brane position

  36. The model parameters: Φ IR Φ x IR IR brane Φ UV Φ x UV coeff. coeff. 5d value value position value value of M of Φ x coupling set explicit breaking sources = 0 matching to Π V current correlators Π S G^2 term Π V Leading log term Leading log term 3 phenomenological input values Fix F π = 246 GeV/√ N D = 123 GeV (1FM) M Φ = 125 GeV S = 0.1

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