REVIEW
750 GeV Diphoton Signal from One-Family Walking Technipion
High Energy Physics - Phenomenology · Submitted 17 Dec 2015 · 38 references
Pith's verdict: A quick, competent application of the authors' own walking-technicolor machinery to the December 2015 diphoton bump — the arithmetic is right and the rate isn't tuned, but the 'N_C=3 is favored' conclusion rests on an LO cross section sitting at 80% of the 8 TeV limit.
T0 · AI review
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Referee report
The paper
The paper claims
The paper argues that the 750 GeV diphoton excess reported by ATLAS and CMS can be explained by a single predicted composite pseudoscalar of the one-family walking technicolor model, whose couplings to gluons and photons are fixed by the QD
The reading
What carries the argument
The load-bearing mechanism is the Wess-Zumino-Witten anomaly term of the chiral Lagrangian for the one-family model, which fixes the $P^0$ couplings to $g g$, $%5Cgamma%5Cgamma$, $Z%5Cgamma$ and $ZZ$ in terms of the technipion decay constant and the number of technicolors, with no adjustable strength. The central object is the singlet pseudoscalar $P^0 %5Csim (1/(4%5Csqrt{3}))(%5Cbar{Q} i%5Cgamma_5 Q - 3%5Cbar{L} i%5Cgamma_5 L)$, the one technipion whose couplings are not suppressed by the techniquark-technilepton cancellation that kills the $P^0 WW$ vertex. Because all partial widths carry the same $N_C^2$ factor, the branching ratios are $N_C$-independent and the only remaining dial is the mass.
Extended reading notes
Core claim
The claim is that the iso- and color-singlet technipion $P^0$ of the one-family walking technicolor model, taken at a mass of 750 GeV, reproduces the observed diphoton rate. The model has $N_F=8$ technifermions (three techniquarks carrying color and a technilepton doublet), so the chiral symmetry is $SU(8)_L imes SU(8)_R$ broken to $SU(8)_V$, giving 63 pseudoscalars of which three are eaten by $W$ and $Z$. The remaining 60 technipions get mass from extended technicolor and Standard Model gauge interactions, lifted to the TeV scale by the large anomalous dimension of the walking dynamics. The singlet combination $P^0$ couples to gauge bosons only through the non-Abelian anomaly, with the decay constant fixed to $F_%5Cpi = v_{m EW}/%5Csqrt{N_D} = 123$ GeV. Every partial width scales as $N_C^2$, so the branching ratios are independent of $N_C$: at 750 GeV the state is 99.8 percent digluon, $9.7 imes 10^{-2}$ percent diphoton, $5.3 imes 10^{-2}$ percent $Z%5Cgamma$ and $7.3 imes 10^{-3}$ percent $ZZ$, with $P^0 o WW$ forbidden by cancellation between techniquark and technilepton loops. With CTEQ6L1 parton densities and the narrow-width approximation, gluon fusion at 13 TeV gives about $7.7 imes 10^3$ fb in digluons and 7.5 fb in diphotons for $N_C=3$ (13 fb for $N_C=4$). Checking against 8 TeV limits, the $N_C=4$ diphoton rate of 2.9 fb sits above the quoted bound of 2.0 fb, while $N_C=3$ at 1.6 fb survives, so the authors conclude that $N_C=3$ is the favored case. They note as an open caveat that extended-technicolor Yukawa couplings, especially to the top, could interfere with the anomaly amplitude and shift the branching fractions.
Load-bearing premise
The $P^0$ mass is put in by hand at 750 GeV, while the paper itself says extended technicolor and Standard Model gauge interactions push technipion masses to the TeV scale, so nothing here explains why this particular state should sit at 750 GeV rather than higher.
Editorial extensions
If this is right
- Run-II data should show correlated excesses near 750 GeV in dijets, $Z%5Cgamma$ and $ZZ$, in the ratios implied by the branching fractions: roughly 7.7 pb in digluons, 4.1 fb in $Z%5Cgamma$ and 0.56 fb in $ZZ$ at 13 TeV for $N_C=3$.
- The $N_C=4$ version of the model is disfavored, since its 8 TeV diphoton rate of 2.9 fb exceeds the quoted 95 percent C.L. bound of 2.0 fb, leaving $N_C=3$ as the consistent choice.
- The same model keeps its other predictions intact: a 125 GeV technidilaton matching the Higgs couplings and a technirho near 2 TeV matching the ATLAS diboson excess.
- The resonance should be narrow, with a total width of order 1 GeV, consistent with the interpretation of the diphoton bump as a single particle rather than a broad effect.
Reading between the lines
- Because 99.8 percent of the decays go to two gluons, this state is a dijet resonance first and a diphoton resonance second; any anomaly-coupled explanation of a 750 GeV photon bump inherits a much larger jet signal that is the sharper place to look.
- The anomaly fixes the relative rates across channels, so the ratios $Z%5Cgamma : %5Cgamma%5Cgamma : ZZ %5Capprox 0.55 : 1 : 0.075$ are a stronger test than the diphoton rate alone, since a common overall normalization cannot rescue a mismatch in the pattern.
- The mass is the one quantity the paper does not derive; a lattice or extended-technicolor calculation of the technipion mass splitting that lands near 750 GeV would turn this from an accommodation into a prediction, and one that lands near 1 TeV would end it.
- If the singlet exists, the QCD-colored technipions should lie nearby in mass and decay into dijets or top pairs, giving an independent handle that does not rely on the photon channel at all.
Original abstract
The ATLAS and CMS groups have recently reported an excess at around 750 GeV with the local significance by about 3 sigma in the diphoton channel at the 13 TeV LHC. We give a possible explanation for the excess by a composite pseudo scalar $(P^0)$ predicted in the one-family model of walking technicolor.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
The ATLAS and CMS groups have recently reported an excess at around 750 GeV with the local significance by about 3 sigma in the diphoton channel at the 13 TeV LHC. We give a possible explanation for the excess by a composite pseudo scalar $(P^0)$ predicted in the one-family model of walking technicolor.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The ATLAS and CMS groups have recently reported an excess at around 750 GeV with the local significance by about 3 sigma in the diphoton channel at the 13 TeV LHC. | background 1.00 | 0.04 | 0.05 | asserted 0.95 |
| s1 | We give a possible explanation for the excess by a composite pseudo scalar $(P^0)$ predicted in the one-family model of walking technicolor. | contribution 0.87 | 0.75 | 0.78 | hedged possibility 0.98 |
What was examined, and what was not
- arXiv listing abstract v2
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- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
References
How the literature uses it
64 arXiv papers cite this in 73 sentences
Papers citing it · 28 sentences without a confident label
Uses its data or values 1 paper
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In the one-family walking technipion model discussed recently in Ref. [ref] (see also references therein) the partial $gg$ and $γγ$ decay widths are given as:
Can the diphoton enhancement at 750 GeV be due to a neutral technipion? · One-family walking technicolor model · 0.88
Compares with it 1 paper
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The models we consider here are qualitatively different from other proposals in the literature [ref] because our scenario provides, at the same time, a composite pNGB Higgs and top partners (thus addressing the hierarchy problem), as well as minimality (only the WZW interactions are needed).
Singlets in Composite Higgs Models in light of the LHC di-photon searches · Introduction · 0.97
Cites it as background 43 papers
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This could be an argument against the reality of the diphoton excess, meaning nothing but a statistical fluctuations; but if taken seriously, it put strong constraint on the implied model building [ref] [ Refs. [ref] on this subject appeared at the same time as this work.].
The Minimal Scalar-Stealth Top Interpretation of the Diphoton Excess · Introduction · 0.85
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Although many attempts [ref] have already been made in the context of a scalar resonance coupled to vector-like fermions, our prime goal in this paper is to show that the vector-like fermions assisting the production and decay of the scalar can be related to a possible dark sector.
750 GeV Di-photon excess at CERN LHC from a dark sector assisted scalar decay · Introduction · 0.81
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Subsequently a vast of paper along this line of issue has been arisen in Ref. [ref] .
Four-loop Neutrino Model Inspired by Diphoton Excess at 750 GeV · Introduction · 0.98
What it cites · 34 sentences without a confident label
Uses the method or tool of 1 paper
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The coupling form can unambiguously be fixed by the Wess-Zumino-Witten construction [ref] in terms of the chiral Lagrangian just like the case of QCD pions [ref] : [equation] where things have been written in terms of differential forms on the Minkowski-space manifold $M^4$, and $e, s_W, g_s$ and $F_π$ respectively denote the electromagnetic coupling, weak mixing angle $(s_W ≡sinθ_W, c_W^2≡1- s_W^2)$, the QCD gauge coupling, and the technipion decay constant fixed by the electroweak scale $v_EW=246$ GeV as $F_π= v_EW/√(N_D)$, with $N_D=N_F/2=4$ for the one-family model.
Walking techni-pions at LHC · Introduction · 0.87
Discussion
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