2020
DOI: 10.1016/j.physletb.2020.135448
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Search for dijet resonances using events with three jets in proton-proton collisions at s=13TeV

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Cited by 17 publications
(15 citation statements)
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“…Figure 4: Upper limits at 95% CL on the universal quark coupling g q ', as a function of resonance mass, for a narrow vector resonance that only couples to quarks. The observed limits (solid curve), expected limits (dashed curve) and their variation (shaded bands) are shown [7].…”
Section: Intermediate Mass Regime -Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Figure 4: Upper limits at 95% CL on the universal quark coupling g q ', as a function of resonance mass, for a narrow vector resonance that only couples to quarks. The observed limits (solid curve), expected limits (dashed curve) and their variation (shaded bands) are shown [7].…”
Section: Intermediate Mass Regime -Resultsmentioning
confidence: 99%
“…The main background originates from QCD multijet events (t-channel production). This analysis [7] is using a special data-taking technique called data scouting, which consists of saving only the calorimeter-based jets reconstructed by the software trigger system in CMS, allowing the analysis of much larger rate of data. In order to increase sensitivity to even lower resonance masses with respect to the trigger requirements, this search selects events with at least three jets in the final state.…”
Section: Intermediate Mass Regime -Resolved Dijet Searchmentioning
confidence: 99%
“…It may be possible to put a bound on σ ϕ ðM ϕ Þ from the dijet resonance searches. For example, the one performed by the CMS Collaboration at the 13 TeV LHC [80] indicates that σ ϕ × BRðϕ → ggÞ has to be less than about 1 pb for M ϕ ¼ 1 TeV and about 20 pb for M ϕ ¼ 600 GeV. Similarly, in the quark mode, σ ϕ ×BRðϕ → dd þ ss þ bbÞ is less than about 1 pb for M ϕ ¼ 1 TeV and about 5 pb for M ϕ ¼ 600 GeV.…”
Section: Prospects At the Lhcmentioning
confidence: 99%
“…Studies of this kind were among the first published using early data from the ATLAS [1][2][3][4] and CMS [5][6][7] experiments at the Large Hadron Collider (LHC) at CERN, when operations at high energy first began. Later results used new datasets as the LHC increased the collision energy, from 7 TeV to 8 TeV during Run 1 [8][9][10], and then to 13 TeV for Run 2 [11][12][13][14][15][16][17][18]. Typically, these searches initially focused on resonances with high dijet invariant masses, m jj , e.g.…”
Section: Introductionmentioning
confidence: 99%