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[ref] by taking into account efficiency and acceptance, see for instance, the footnote 1 in Ref. [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"1601.07167","title":"Photo-production of a 750 GeV di-photon resonance mediated by Kaluza-Klein leptons in the loop","url":"/paper/1601.07167","section":"Introduction","sentence":"The cross-sections for the observed di-photon excess were estimated in Ref. [ref] (see also Refs. [ref] ) as [equation] which we will take to be 8 fb.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1512.07885","title":"LHC diphoton excess from colorful resonances","url":"/paper/1512.07885","section":"Diphoton signal from cascade decay of $G'$","sentence":"This estimation is coming from the fact that for either short ($Γ_γγ=5$ GeV) or broad ($Γ_γγ=45$ GeV) diphoton resonance, the $2σ$ region for signal cross-section is between $[1,11 ]$ fb [ref] .","intent_p":0.86,"contests_p":null},{"arxiv_id":"1606.06375","title":"Diphotons at the $Z$-pole in Models of the 750 GeV Resonance Decaying to Axion-Like Particles","url":"/paper/1606.06375","section":"Total width","sentence":"As mentioned in the Introduction, we will consider two scenarios inspired by the fitting of the data performed in [ref] : (1) a wide scenario with $σ_γγ^13TeV=6$ fb and $Γ_S=40$ GeV, (2) a narrow scenario with $σ_γγ^13TeV=2.5$ fb and $Γ_S=5$ GeV.","intent_p":0.97,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":4,"sentences":6,"quotes":[{"arxiv_id":"1601.00006","title":"How Resonance-Continuum Interference Changes 750 GeV Diphoton Excess: Signal Enhancement and Peak Shift","url":"/paper/1601.00006","section":"Dataset and Method","sentence":"Our read-in data and model-independent fit results without interferences approximately agree with those in Ref. 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[ref] ; in particular in terms of the best-fit cross sections for the anomaly.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1604.01008","title":"Diphoton excess and VV-scattering","url":"/paper/1604.01008","section":"$γγ$ scattering","sentence":"[ref] only considers gluon fusion dominated production and takes large QCD $k$-factors into account, in their notation $c_Sγγ = v/m_Sκ_γ/16π^2$, where $v$ is the Higgs vev.].","intent_p":0.89,"contests_p":null},{"arxiv_id":"1603.08932","title":"Diphotons from an Electroweak Triplet-Singlet","url":"/paper/1603.08932","section":"Introduction","sentence":"Since the SM Higgs remains the only source of spontaneous EWSB, this scenario is intrinsically different from models where the neutral component of an $SU(2)_L$ doublet is responsible for the diphoton excess [ref] , as well as from left-right symmetric approaches to the diphoton excess [ref] or Georgi-Machacek models [ref] , in which an EW triplet acquires a vev, and from extensions of $SU(2)_L$ [ref] .","intent_p":0.81,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1604.01008","title":"Diphoton excess and VV-scattering","url":"/paper/1604.01008","section":"Introduction","sentence":"Direct couplings to standard fermions and the Higgs must be suppressed as no fermion final state has been observed and the mixing with the Higgs is severely constrained [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1606.04131","title":"Bounds on supersymmetric effective operators from heavy diphoton searches","url":"/paper/1606.04131","section":"Motivation","sentence":"This is actually welcome for minimal supersymmetric models (MSSM, etc) where it is not possible to have a heavy resonance $X$ with such significant $σ$ [ref] , except if[ Many non-supersymmetric explanations were reported for this 750 GeV “resonance”, see [ref] for a long list of references. $X$ was a scalar singlet with couplings to new TeV states that mediate (at loop level) its production by $gg$ fusion and its decay to $γγ$ [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1605.07962","title":"Cornering diphoton resonance models at the LHC","url":"/paper/1605.07962","section":"Introduction","sentence":"We further assume that the new resonance does not mix with the SM Higgs boson, as existing and projected limits from Higgs coupling measurements set strong indirect constraints [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":72,"sentences":77,"quotes":[{"arxiv_id":"1512.07243","title":"Asymmetric Dark Matter in the Sun and the Diphoton Excess at the LHC","url":"/paper/1512.07243","section":"Introduction","sentence":"Although the significance of this excess is only around $3 σ$ and more statistics is required to draw a firm conclusion, it has already triggered an avalanche of theoretical speculations in terms of a new resonance $X$; see e.g. [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"1601.01571","title":"A 750 GeV Portal: LHC Phenomenology and Dark Matter Candidates","url":"/paper/1601.01571","section":"Two Different Scenarios for","sentence":"Related studies considering gluon fusion partonic processes have been recently performed in Refs. [ref] , whereas photon fusion was considered in Refs. 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