2018
DOI: 10.1103/physrevd.98.112014
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Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at s=13TeV

Abstract: A general search for the pair production of resonances, each decaying to two quarks, is reported. The search is conducted separately for heavier resonances (masses above 400 GeV), where each of the four final-state quarks generates a hadronic jet resulting in a four-jet signature, and for lighter resonances (masses between 80 and 400 GeV), where the pair of quarks from each resonance is collimated and reconstructed as a single jet resulting in a two-jet signature. In addition, a b-tagged selection is applied t… Show more

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Cited by 41 publications
(41 citation statements)
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“…Gluinos must be heavier than 1.5 (1.4) TeV [86,87] for decays into 2 (4) jets. 3 Searches for R-parity violating top squark decays by CMS [89] and ATLAS [87,[96][97][98] put complementary constraints on triplets decaying to two jets, that depend upon whether one of the jets is tagged for b quarks: mt > 520 GeV for decays into first or second generation quarks qq, versus mt > 610 GeV for decays into bq. Table II shows that one must take rather large values of the couplings λ SΦ , λ HΦ to satisfy the collider limits on m Φ .…”
Section: Fitting the Anomaliesmentioning
confidence: 99%
“…Gluinos must be heavier than 1.5 (1.4) TeV [86,87] for decays into 2 (4) jets. 3 Searches for R-parity violating top squark decays by CMS [89] and ATLAS [87,[96][97][98] put complementary constraints on triplets decaying to two jets, that depend upon whether one of the jets is tagged for b quarks: mt > 520 GeV for decays into first or second generation quarks qq, versus mt > 610 GeV for decays into bq. Table II shows that one must take rather large values of the couplings λ SΦ , λ HΦ to satisfy the collider limits on m Φ .…”
Section: Fitting the Anomaliesmentioning
confidence: 99%
“…There are some relevant LHC searches in this case. For example the CMS search for pair-produced resonances decaying into quark pairs [100] is relevant for constraining the HA pair production. However, the QCD backgrounds for this process completely overwhelm the weak scale production of the Δm (GeV) Figure 7: The bounds for v t = 10 −4 GeV from invisible Higgs branching fraction [94][95][96][97] and the LEP chargino searches [102].…”
Section: ∆M <mentioning
confidence: 99%
“…For the heaviest scalars the production and decay chain is pp → H 3,4 → H 2 H 2 , with subsequent decay of H 2 . A search for pair produced resonances decaying into quark pairs by the CMS Collaboration [56] is sensitive to (but no optimised for) this process. The limits corresponding to stop masses mt = 80 GeV are σ(tt * ) ≤ 400 pb, assuming 100% branching ratio for the R-parity violating decayt → bq.…”
Section: Scenariomentioning
confidence: 99%