Title: Phenomenology Beyond the Standard Model
1STANDARD MODEL
2There must be New Physics Beyond the Standard
Model
viXra Bloggers Combination of Dec.13th Data
Precision Electroweak data?? Higgs coupling blows
up!!
Higgs coupling less than in Standard Model
Higgs potential collapses
3Theorists getting Cold Feet
- Composite Higgs model?
- conflicts with precision electroweak data
- Interpretation of EW data?
- consistency of measurements? Discard some?
- Higgs higher-dimensional operators?
- corridors to higher Higgs masses?
- Little Higgs models?
- extra Top, gauge bosons, Higgses
- Higgsless models?
- strong WW scattering, extra D?
4Heretical Interpretation of EW Data
Do all the data tell the same story? e.g., AL vs
AH
What most of us think
Chanowitz
5Estimates of mH from different Measurements
Spread looks natural no significant disagreement
6Higgs Higher-Order Operators
Corridor to heavy Higgs?
Precision EW data suggest they are small why?
Do not discard possibility of heavy Higgs
Barbieri, Strumia
7(No Transcript)
8Elementary Higgs or Composite?
- Higgs field
- lt0H0gt ? 0
- Quantum loop problems
- Fermion-antifermion condensate
- Just like QCD, BCS superconductivity
- Top-antitop condensate? needed mt gt 200 GeV
Cutoff ? 10 TeV
- New technicolour force?
- Heavy scalar resonance?
- Inconsistent with
- precision electroweak data?
Cut-off ? 1 TeV with Supersymmetry?
9Comparison between Weakly- and Strongly-coupled
Models
10Interpolating Models
- Combination of Higgs boson and vector ?
- Two main parameters m? and coupling g?
- Equivalently ratio weak/strong scale
- g? / m?
Grojean, Giudice, Pomarol, Rattazzi
11Intermediate Models
12Effects on Higgs Decays
- Dependences on ? of Higgs branching ratios
- Standard Model recovered in limit ??0
Grojean, Giudice, Pomarol, Rattazzi
13Higgs as a Pseudo-Goldstone Boson
Little Higgs models (breakdown of larger
symmetry)
Loop cancellation mechanism
Supersymmetry
Little Higgs
14Little Higgs Models
- Embed SM in larger gauge group
- Higgs as pseudo-Goldstone boson
- Cancel top loop
- with new heavy T quark
-
- New gauge bosons, Higgses
- Higgs light, other new
- physics heavy
MT lt 2 TeV (mh / 200 GeV)2 MW lt 6 TeV (mh / 200
GeV)2 MH lt 10 TeV
Not as complete as susy more physics gt 10 TeV
15Examples of Higgs as Pseudo-Goldstone Boson
- Parameterization of effective Lagrangian
- Examples
- To be measured!
16What if the Higgs is not quite a Higgs?
- Tree-level Higgs couplings masses
- Coefficient 1/v
- Couplings dilaton of scale invariance
- Broken by Higgs mass term µ2, anomalies
- Cannot remove µ2 (Coleman-Weinberg)
- Anomalies give couplings to ??, gg
- Generalize to pseudo-dilaton of new (nearly)
conformal strongly-interacting sector - Pseudo-Goldstone boson of scale symmetry
17A Phenomenological Profile of a Pseudo-Dilaton
- Universal suppression of couplings to Standard
Model particles a c v/V - Effective potential
- Self-couplings
- G(gg) may be enhanced
- G(??) may be suppressed
Compilation of constraints
Updated with Dec. 11 constraints
Pseudo-baryons as dark matter?
Campbell, JE, Olive arXiv1111.4495
18General Analysis of Less Higgs Models
- Parameterization of effective Lagrangian
- Fits
a ? c
Azatov, Contino, Galloway arXiv1202.3415
Espinosa, Grojean, Muhlleitner, Trott
arXiv1202.3697
19General Analysis of Less Higgs Models
- Separate fits to CMS and ATLAS data
Azatov, Contino, Galloway arXiv1202.3415
20Sum Rule for More or Less Higgs Models
- What if Higgs-V-V couplings differ from SM?
- Unitarity imposes sum rule on scattering in
different isospin channels - If Higgs coupling gt Standard Model (a2 gt 1), must
have non-zero scattering with I 2
Fialkowski, Rychkov, Urban arXiv1202.1532
21Higgsless Models?
- Four-dimensional versions
- Strong WW scattering _at_ TeV, incompatible with
precision data? - Break EW symmetry by boundary conditions in extra
dimension - delay strong WW scattering to 10 TeV?
- Kaluza-Klein modes mKK gt 300 GeV?
- compatibility with precision data?
- Warped extra dimension brane kinetic terms?
Lightest KK mode _at_ few 00 GeV, strong WW _at_ 6-7
TeV
22Particle Spectrum in Simplest Model with Extra
Dimensions
- Lowest-lying states have flat wave functions (n
0) - Excitations (Kaluza-Klein) have nodes (n gt 0)
- Mass n/R (R radius of circle)
23Fold Circle Orbifold
- Identify two halves of circle up to a minus sign
- Even particles include massless odd ones all
massive - A way to give masses to particles that are
asymmetric
24Mechanism to break Gauge Symmetry
- Identify two halves up to a group transformation
U - Unbroken part of gauge group commutes with U
- Masses for asymmetric particles
- e.g., SU(2) U(1) ? U(1)
25Search for Vector Resonance in Higgsless Model
- Vector resonance structure in WZ scattering
Simulation of resonance structure in mWZ _at_ LHC