2012
DOI: 10.1007/jhep11(2012)097
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Probing colored particles with photons, leptons, and jets

Abstract: If pairs of new colored particles are produced at the Large Hadron Collider, determining their quantum numbers, and even discovering them, can be non-trivial. We suggest that valuable information can be obtained by measuring the resonant signals of their near-threshold QCD bound states. If the particles are charged, the resulting signatures include photons and leptons and are sufficiently rich for unambiguously determining their various quantum numbers, including the charge, color representation and spin, and … Show more

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Cited by 37 publications
(59 citation statements)
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“…2) applies in all cases of dominant three body final state. We conclude that the search for bound states is truly a generic tool to look for exotic colored scalars [4]. The quantum numbers of X determine the gluon fusion (ggF) production cross section of S as well as its decay rates into pairs of vector bosons: gg, γγ, ZZ, Zγ and W W .…”
Section: Qcd Bound Statementioning
confidence: 96%
See 2 more Smart Citations
“…2) applies in all cases of dominant three body final state. We conclude that the search for bound states is truly a generic tool to look for exotic colored scalars [4]. The quantum numbers of X determine the gluon fusion (ggF) production cross section of S as well as its decay rates into pairs of vector bosons: gg, γγ, ZZ, Zγ and W W .…”
Section: Qcd Bound Statementioning
confidence: 96%
“…For example, as demonstrated by the non-degenerate quartet scenario (case B in section 5), the data still allow four colored states with m X 250 GeV. In this section we study another way to discover light colored scalars, which might go first through the observation of their QCD bound state [4,5,68]. Moreover, constraints derived from bound state searches are less model dependent, in the sense that they do not depend on the decay mode of X.…”
Section: Qcd Bound Statementioning
confidence: 99%
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“…Our analysis relies on a number of previous works [41][42][43][44][45][46][47][48][49][50], notably those of Martin and collaborators [51][52][53][54]. Next we describe in more detail the basic requirements for observable stoponium annihilation decays.…”
Section: Jhep07(2015)061mentioning
confidence: 99%
“…This removes LHC constraints on the stop mass (see e.g. [61]), reducing the tension between LHC results and naturalness. Nonetheless, our model is also viable with R-parity conservation.…”
Section: Jhep10(2014)182mentioning
confidence: 99%