the 750 gev excess from photon-photon and quark-quark...
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The 750 GeV excess from photon-photon The 750 GeV excess from photon-photon and quark-quark processesand quark-quark processes
Tanumoy Mandal
In collaboration with U. Danielsson, R. Enberg, G. Ingelman Based on arXiv:1601.00624
(Moriond QCD, March 20, 2016)
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IntroductionExcess is only seen in the diphoton channel
Resonance may couple dominantly to photonsCoupling to gluons can be suppressed or absent
A photon-philic resonance?
A lot of model buildings and proposals to explain the resonance
310 papers by the June 1, 2016
“A Theory of Ambulance Chasing” predicted[1603.01204]
(Possibly no hard activities associated with diphoton)
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Run-I vs Run-II data
Serious tension
Non-observation in Run-I data
Observationin Run-II data
A generic s-channel production
For background
Tension in the photon-fusion channel is slightly reduced
Using NN23LO PDF
Ratio of signal events in Run-I and Run-II: Compatibility ratio
A slight upwardfluctuation around 750 GeV
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Photon fusion
1512.05751;1512.05776;1512.08502;1601.00386;1601.00638;1601.01144;1601.01571;1601.01712;1601.03772;1601.07167;1601.07187;1602.02380;1602.07574;1601.07774;1603.00287 ... more
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Uncertainties in photon-fluxPhoton-fusion contribution can be very large due to IR enhancement in the collinear limit (equivalent / Weizsacker-Williams photon approximation)
Various uncertainties
Elastic photon-flux Inelastic photon-flux
Cross section crucially depends on the proton form-factors
In the forward limit, IR singularities are cutoff by the finite size of the proton
Leading order computation is not a good approximation and one should takeinto account the large collinear logarithms properly for robust predictions
Due to these uncertainties Run-I data might be compatible to the Run-II data
Compatibility ratio can vary a lot
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Examples of uncertaintiesC. Csaki, J. Hubisz, S. Lombardo, J. Terning [1601.00638]
M. Ababekri, S. Dulat, J. Isaacson, C. Schmidt, C. P. Yuan [1603.04874]
Why so different? Need to understand various issues in the photon-flux
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Quark fusion
An extra hard photon in the final stateSignificant fraction of events survive after selection cuts
Basic quark-fusion topologyDiphoton associated with an extra hard jet. Higher-order correction to s-channel ggF
1512.068331601.00624
1512.04933;1512.08478;1603.03421;1603.04248... more
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Varying EM couplingSpace-time varying EM coupling
Proposed by Jacob Bekenstein: a scalar with tiny mass [PRD 25, 1527 ('82)]
Mass is free (we choose 750 GeV). OK with cosmology
Only one free parameter. No new particle is required
A very “economical” and “predictive” model
This scalar does not couple to gg, photon-Z, ZZ or WW
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Decay modes
BRs are independent of scale, only depends on mass
Diphoton BR is as large as 68% (a photon-philic scalar)
Total width can be large depending on ,
s-channel gluon-fusion is not present in this model
Tree-level effective vertex, no loop suppression
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Productionst-channel contaminationcan be neglected safely
Due to various uncertainties total photon-fusion x-sec vary a lot
Work in progress @ THEP group, Uppsala university
Extra hard photon orjets in the final state
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Distributions
Disfavoredfrom data?
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Recast limit
To recast x-sec upper limit, one should take care cut-efficiencies
i=all processescontributing toan experiment
Searches are optimized for an s-channel resonance
Inclusion of elastic+inelastic photon-fusion contributions would modify the scale
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Conclusions/OutlooksA photon-philic (68% BR) scalar is present in this model
Economical: one free parameter, no new particles needed
vertex is not loop-suppressed, large production rate
Total width can be large, about 12 GeV for TeV
Observed excess can be explained for TeV
Distinct signatures: a hard third photon (roughly in 40% events), resonance in mass distribution (22% BR)
Important to understand various uncertainties involved in the photon-fusion productions (work in progress)
THE ELECTROMAGNETIC-FORCE AWAKENS NOW?
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