• • • We do not use the following data for averages, fits, limits, etc. • • • |
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<2603
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95
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200
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<44
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95
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<7
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95
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1
AABOUD 2019AJ search for low mass dijet resonance in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit X}}$ , ${{\mathit X}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ at 13 TeV with 79.8 fb${}^{-1}$ of data; no signal found; limits placed on ${{\mathit Z}^{\,'}}$ model in coupling vs. m(${{\mathit Z}^{\,'}}$) plane.
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SIRUNYAN 2019B search for low mass resonance ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit A}}$ , ${{\mathit A}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ at 13 TeV using 35.9 fb${}^{-1}$; no signal; exclude resonances $50 - 350$ GeV depending on production and decay.
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3
SIRUNYAN 2019CD search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}{{\mathit \gamma}}$ , ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ with fat jet ( ${{\mathit j}}{{\mathit j}}$ ); no signal, limits placed in m(${{\mathit Z}^{\,'}}$) vs. coupling plane for ${{\mathit Z}^{\,'}}$ masses from 10 to 125 GeV.
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4
AABOUD 2018AD search for new heavy particle ${{\mathit Y}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ $\rightarrow$ ( ${{\mathit b}}{{\mathit b}}$) ${+}$ ( ${{\mathit q}}{{\mathit q}}$). No signal observed. Limits set on m(Y) vs. m(X) in the ranges of m(Y) in $1 - 4$ TeV and m(X) in $50 - 1000$ GeV.
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5
AABOUD 2018CK search for SUSY Higgsinos in gauge-mediation via ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\mathit b}}{{\mathit b}}$ + $\not E_T$ at 13 TeV using two complementary analyses with 24.3/36.1 fb${}^{-1}$; no signal is found and Higgsinos with masses between 130 and 230 GeV and between 290 and 880 GeV are excluded at the 95$\%$ confidence level.
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6
AABOUD 2018CL search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ vector-like quarks $\rightarrow$ jets at 13 TeV with 36 fb${}^{-1}$; no signal seen; limits set on various VLQ scenarios. For pure ${{\mathit B}}$ $\rightarrow$ ${{\mathit H}}{{\mathit b}}$ or ${{\mathit T}}$ $\rightarrow$ ${{\mathit H}}{{\mathit t}}$ , set the mass limit m $>$ 1010 GeV.
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7
AABOUD 2018N search for dijet resonance at Atlas with 13 TeV and 29.3 fb${}^{-1}$; limits set on m(${{\mathit Z}^{\,'}}$) in the mass range of $450 - 1800$ GeV.
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8
SIRUNYAN 2018DJ search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ or ${{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}{{\mathit j}}{{\mathit j}}$ resonance at 13 TeV, 35.9 fb${}^{-1}$; no signal; limits set in the $400 - 4500$ GeV mass range, exclusion of ${{\mathit W}^{\,'}}$ up to 2270 GeV in the HVT model A, and up to 2330 GeV for HVT model B. WED bulk graviton exclusion up to 925 GeV.
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9
SIRUNYAN 2018DY search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit R}}{{\mathit R}}$ ; ${{\mathit R}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ two dijet resonances at 13 TeV 35.9 fb${}^{-1}$; no signal; limits placed on RPV top-squark pair production.
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10
KHACHATRYAN 2017W search for dijet resonance in 12.9 fb${}^{-1}$ data at 13 TeV; see Fig. 2 for limits on axigluons, diquarks, dark matter mediators etc.
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KHACHATRYAN 2017Y search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ($8 - 10)~{{\mathit j}}$ in 19.7 fb${}^{-1}$ at 8 TeV. No signal seen. Limits set on colorons, axigluons, RPV, and SUSY.
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SIRUNYAN 2017F measure ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ angular distribution in 2.6 fb${}^{-1}$ at 13 TeV; limits set on LEDs and quantum black holes.
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13
AABOUD 2016 search for resonant dijets including one or two ${{\mathit b}}$-jets with 3.2 fb${}^{-1}$ at 13 TeV; exclude excited ${{\mathit b}^{*}}$ quark from $1.1 - 2.1$ TeV; exclude leptophilic ${{\mathit Z}^{\,'}}$ with SM couplings from $1.1 - 1.5$ TeV.
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14
AAD 2016N search for ${}\geq{}$3 jets with 3.6 fb${}^{-1}$ at 13 TeV; limits placed on micro black holes (Fig. 10) and string balls (Fig. 11).
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AAD 2016S search for high mass jet-jet resonance with 3.6 fb${}^{-1}$ at 13 TeV; exclude portions of excited quarks, ${{\mathit W}^{\,'}}$, ${{\mathit Z}^{\,'}}$ and contact interaction parameter space.
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KHACHATRYAN 2016K search for dijet resonance in 2.4 fb${}^{-1}$ data at 13 TeV; see Fig. 3 for limits on axigluons, diquarks etc.
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KHACHATRYAN 2016L use data scouting technique to search for ${{\mathit j}}{{\mathit j}}$ resonance on 18.8 fb${}^{-1}$ of data at 8 TeV. Limits on the coupling of a leptophobic ${{\mathit Z}^{\,'}}$ to quarks are set, improving on the results by other experiments in the mass range between $500 - 800$ GeV.
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AAD 2013D search for dijet resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.8 fb${}^{-1}$. The observed events are compatible with Standard Model expectation. See their Fig. 6 and Table 2 for limits on resonance cross section in the range $\mathit m$ = $1.0 - 4.0$ TeV.
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AALTONEN 2013R search for production of a pair of jet-jet resonances in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 6.6 fb${}^{-1}$. See their Fig. 5 and Tables I, II for cross section limits.
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CHATRCHYAN 2013A search for ${{\mathit q}}{{\mathit q}}$ , ${{\mathit q}}{{\mathit g}}$ , and ${{\mathit g}}{{\mathit g}}$ resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.8 fb${}^{-1}$. See their Fig. 3 and Table 1 for limits on resonance cross section in the range $\mathit m$ = $1.0 - 4.3$ TeV.
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CHATRCHYAN 2013A search for ${{\mathit b}}{{\overline{\mathit b}}}$ resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.8 fb${}^{-1}$. See their Fig. 8 and Table 4 for limits on resonance cross section in the range $\mathit m$ = $1.0 - 4.0$ TeV.
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22
AAD 2012S search for dijet resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 1.0 fb${}^{-1}$. See their Fig. 3 and Table 2 for limits on resonance cross section in the range = $0.9 - 4.0$ TeV.
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CHATRCHYAN 2012BL search for ${{\mathit t}}{{\overline{\mathit t}}}$ resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.4 fb${}^{-1}$. See their Fig. 4 for limits on resonance cross section in the range $\mathit m$ = $0.5 - 3.0$ TeV.
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AAD 2011AG search for dijet resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with L = 36$~$pb${}^{-1}$. Limits on number of events for $\mathit m$ = $0.6 - 4$ TeV are given in their Table 3.
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AALTONEN 2011M find a peak in two jet invariant mass distribution around 140 GeV in ${{\mathit W}}$ + 2 jet events in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96$~$TeV with L = 4.3 fb${}^{-1}$.
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26
ABAZOV 2011I search for two-jet resonances in ${{\mathit W}}$ + 2 jet events in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96$~$TeV with L = 4.3 fb${}^{-1}$ and give limits $\sigma <$ ($2.6 - 1.3$) pb (95$\%$ CL) for $\mathit m$ = $110 - 170$ GeV. The result is incompatible with AALTONEN 2011M.
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AAD 2010 search for narrow dijet resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with L = 315$~$nb${}^{-1}$. Limits on the cross section in the range $10 - 10^{3}$ pb is given for ${\mathit m}_{\mathrm {}}$ = $0.3 - 1.7~$TeV.
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KHACHATRYAN 2010 search for narrow dijet resonances in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7$~$TeV with L = 2.9 pb${}^{-1}$. Limits on the cross section in the range $1 - 300$ pb is given for ${\mathit m}_{\mathrm {}}$ = $0.5 - 2.6~$TeV separately in the final states ${{\mathit q}}{{\mathit q}}$ , ${{\mathit q}}{{\mathit g}}$ , and ${{\mathit g}}{{\mathit g}}$ .
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29
ABE 1999F search for narrow ${{\mathit b}}{{\overline{\mathit b}}}$ resonances in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}=1.8$ TeV. Limits on $\sigma\mathrm {( {{\mathit p}} {{\overline{\mathit p}}} \rightarrow {{\mathit X}} + {\mathrm {anything}})}{\times }$B( ${{\mathit X}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ) in the range $3 - 10^{3}~$pb (95$\%$CL) are given for ${\mathit m}_{{{\mathit X}}}=200 - 750$ GeV. See their Table$~$I.
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ABE 1997G search for narrow dijet resonances in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions with 106$~$pb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = $1.8$ TeV. Limits on $\sigma $( ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit X}}$ + anything)$\cdot{}$B( ${{\mathit X}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ ) in the range $~$pb (95$\%$CL) are given for dijet mass $\mathit m=200 - 1150$ GeV with both jets having $\vert {{\mathit \eta}}\vert <2.0$ and the dijet system having $\vert $cos $\theta {}^{*}\vert <0.67$. See their Table$~$I for the list of limits. Supersedes ABE 1993G.
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ABE 1993G give cross section times branching ratio into light (${{\mathit d}}$, ${{\mathit u}}$, ${{\mathit s}}$, ${{\mathit c}}$, ${{\mathit b}}$) quarks for $\Gamma $ = $0.02~\mathit M$. Their Table$~$II gives limits for $\mathit M$ = $200 - 900$ GeV and $\Gamma $ = ($0.02 - 0.2)~\mathit M$.
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