2018
DOI: 10.1007/jhep08(2018)130
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Search for narrow and broad dijet resonances in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV and constraints on dark matter mediators and other new particles

Abstract: Searches for resonances decaying into pairs of jets are performed using proton-proton collision data collected at √ s = 13 TeV corresponding to an integrated luminosity of up to 36 fb −1 . A low-mass search, for resonances with masses between 0.6 and 1.6 TeV, is performed based on events with dijets reconstructed at the trigger level from calorimeter information. A high-mass search, for resonances with masses above 1.6 TeV, is performed using dijets reconstructed offline with a particle-flow algorithm. The dij… Show more

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Cited by 175 publications
(234 citation statements)
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“…The scans were performed over leptoquark couplings y 11 , y 12 , y 21 and y 22 , and the leptoquark mass parameter µ S 3 , with all other couplings fixed. In 2018 the CMS experiment at the LHC set an exclusion on diquark masses below 7.2 TeV at 95% confidence interval [87]. While the exclusion was calculated for a particular diquark which features in superstring inspired E 6 models [88], similar bounds are expected to apply to other diquarks.…”
Section: Resultsmentioning
confidence: 99%
“…The scans were performed over leptoquark couplings y 11 , y 12 , y 21 and y 22 , and the leptoquark mass parameter µ S 3 , with all other couplings fixed. In 2018 the CMS experiment at the LHC set an exclusion on diquark masses below 7.2 TeV at 95% confidence interval [87]. While the exclusion was calculated for a particular diquark which features in superstring inspired E 6 models [88], similar bounds are expected to apply to other diquarks.…”
Section: Resultsmentioning
confidence: 99%
“…) M X to each flavor of quark-antiquark pair, but can also in principle have loop-induced decays to gluon pairs. In particular, they can be produced singly as dijet resonances via qq → X → qq, resulting in the most recent LHC bound of M X > 6.6 TeV assuming g A = g B [80][81][82][83][84][85]. However, in the context of the present paper the bounds will be somewhat weaker if g A < g B , as in the example model of the previous section.…”
Section: Comments On Collider Phenomenologymentioning
confidence: 84%
“…The lightest sgluon mass eigenstate can therefore be produced in gluon fusion and decay to gg (or to tt), leading to a dijet signature for which LHC searches [80][81][82][83][84][85] exist. However, signal/background interference effects can be very large [86] for heavy scalar di-gluon resonances, so that if the di-gluon production and decay dominate, the resonance may manifest as a dip/peak or step-function invariant mass distribution rather than a pure resonance peak.…”
Section: Comments On Collider Phenomenologymentioning
confidence: 99%
“…The red, blue, and green lines correspond to g uu = 0.5, 0.6, and 0.7, respectively. The black line is the observed 95 % CL upper limits with the integrated luminosity, L = 36 fb −1 , at CMS [21]. From the CMS data, the region g uu 0.5 is allowed for m Z ≥ 1 TeV.…”
Section: Dijet Productionmentioning
confidence: 99%
“…The red, blue, and green lines correspond to g uu = 0.5, 0.6, and 0.7, respectively. The black line is the observed 95 % CL upper limits at CMS [21].…”
Section: Triple Top Quark Productionmentioning
confidence: 99%