LIMITS ON JET-JET RESONANCES

Heavy Particle Production Cross Section

INSPIRE  
Limits are for a particle decaying to two hadronic jets.
${\mathrm {Units(pb)}}$ CL$\%$ $\mathit Mass({\mathrm {GeV}}$) DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
1
AAD
2020AD
 ATLS ${{\mathit p}}{{\mathit p}}$ at 13 TeV, dijet resonance
2
AAD
2020T
 ATLS dijet resonance search
3
AAD
2020W
 ATLS dijet resonance plus lepton
4
SIRUNYAN
2020AI
 CMS dijet resonance search
5
AABOUD
2019AJ
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit X}}$ , ${{\mathit X}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
6
SIRUNYAN
2019B
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit A}}$ , ${{\mathit A}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
7
SIRUNYAN
2019CD
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}{{\mathit \gamma}}$ , ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
8
AABOUD
2018AD
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Y}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ $\rightarrow$ ( ${{\mathit b}}{{\mathit b}}$) ${+}$ ( ${{\mathit q}}{{\mathit q}}$)
9
AABOUD
2018CK
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\mathit b}}{{\mathit b}}$ + $\not E_T$
10
AABOUD
2018CL
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ vector-like quarks
11
AABOUD
2018N
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
12
SIRUNYAN
2018DJ
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ or ${{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}{{\mathit j}}{{\mathit j}}$
13
SIRUNYAN
2018DY
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit R}}{{\mathit R}}$ ; ${{\mathit R}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
14
KHACHATRYAN
2017W
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
15
KHACHATRYAN
2017Y
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ($8 - 10$) ${{\mathit j}}$ +$\not E_T$
16
SIRUNYAN
2017F
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ angular distribution
17
AABOUD
2016
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}$ + jet
18
AAD
2016N
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 3 high $\mathit E_{T}$ jets
19
AAD
2016S
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
20
KHACHATRYAN
2016K
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
21
KHACHATRYAN
2016L
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
22
AAD
2013D
 ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
23
AALTONEN
2013R
 CDF 1.96 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 4 jets
24
CHATRCHYAN
2013A
 CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
25
CHATRCHYAN
2013A
 CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit X}}$
26
AAD
2012S
 ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
27
CHATRCHYAN
2012BL
 CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit X}}$
28
AAD
2011AG
 ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
29
AALTONEN
2011M
 CDF 1.96 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit W}}$ + 2 jets
30
ABAZOV
2011I
 D0 1.96 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit W}}$ + 2 jets
31
AAD
2010
ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
32
KHACHATRYAN
2010
CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
33
ABE
1999F
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ + anything
34
ABE
1997G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
$ <2603 $ 95 200 35
ABE
1993G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
$ <44 $ 95 400 35
ABE
1993G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
$ <7 $ 95 600 35
ABE
1993G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
1  AAD 2020AD search for weakly supervised dijet resonance in ATLAS with 139 fb${}^{-1}$ at 13 TeV; no signal; various limits placed depending on kinematics and production cross section.
2  AAD 2020T search for dijet resonance with or without ${{\mathit b}}$ -jets at 13 TeV and 139 fb${}^{-1}$; no signal; limits placed in ${{\mathit \sigma}}$ $\cdot{}$BF vs mass plane for various BSM models.
3  AAD 2020W search for dijet resonance plus lepton with ATLAS at 13 TeV and 139 fb${}^{-1}$; no signal; limits placed in ${{\mathit \sigma}}$ $\cdot{}$BF vs. mass plane for various BSM models.
4  SIRUNYAN 2020AI search for dijet resonance in CMS at 13 TeV with 137 fb${}^{-1}$; no signal; limits set in ${{\mathit \sigma}}$ vs. mass plane for various BSM models .
5  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.
6  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.
7  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.
8  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.
9  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.
10  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.
11  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.
12  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.
13  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.
14  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.
15  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.
16  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.
17  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.
18  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).
19  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.
20  KHACHATRYAN 2016K search for dijet resonance in 2.4 fb${}^{-1}$ data at 13 TeV; see Fig. 3 for limits on axigluons, diquarks etc.
21  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.
22  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.
23  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.
24  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.
25  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.
26  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.
27  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.
28  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.
29  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${}^{-1}$.
30  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.
31  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 pb is given for ${\mathit m}_{\mathrm {}}$ = $0.3 - 1.7~$TeV.
32  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 ${{\mathit g}}{{\mathit g}}$ .
33  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.
34  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.
35  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 $ = ($0.02 - 0.2)~\mathit M$.
References:
AAD 2020W
JHEP 2006 151 Search for dijet resonances in events with an isolated charged lepton using $\sqrt{s} = 13$ TeV proton-proton collision data collected by the ATLAS detector
AAD 2020AD
PRL 125 131801 Dijet resonance search with weak supervision using $\sqrt{s}=13$ TeV $pp$ collisions in the ATLAS detector
AAD 2020T
JHEP 2003 145 Search for new resonances in mass distributions of jet pairs using 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
SIRUNYAN 2020AI
JHEP 2005 033 Search for high mass dijet resonances with a new background prediction method in proton-proton collisions at $\sqrt{s} =$ 13 TeV
AABOUD 2019AJ
PL B795 56 Search for low-mass resonances decaying into two jets and produced in association with a photon using $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
SIRUNYAN 2019B
PR D99 012005 Search for low-mass resonances decaying into bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV
SIRUNYAN 2019CD
PRL 123 231803 Search for low-mass quark-antiquark resonances produced in association with a photon at $\sqrt{s} = $ 13 TeV
AABOUD 2018CL
PR D98 092005 Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
AABOUD 2018N
PRL 121 081801 Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV
AABOUD 2018AD
PL B779 24 A search for resonances decaying into a Higgs boson and a new particle $X$ in the $XH \to qqbb$ final state with the ATLAS detector
AABOUD 2018CK
PR D98 092002 Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector
SIRUNYAN 2018DY
PR D98 112014 Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV
SIRUNYAN 2018DJ
JHEP 1809 101 Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2?2q final states at $ \sqrt{s}=13 $ TeV
KHACHATRYAN 2017W
PL B769 520 Search for Dijet Resonances in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV and Constraints on Dark Matter and other Models
KHACHATRYAN 2017Y
PL B770 257 Search for New Phenomena in Events with High Jet Multiplicity and Low Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
SIRUNYAN 2017F
JHEP 1707 013 Search for New Physics with Dijet Angular Distributions in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
AABOUD 2016
PL B759 229 Search for Resonances in the Mass Distribution of Jet Pairs with One or Two Jets Identified as ${\mathit {\mathit b}}$-Jets in Proton-proton Collisions at $\sqrt {s }$ =13 TeV with the ATLAS Detector
AAD 2016S
PL B754 302 Search for New Phenomena in Dijet Mass and Angular Distributions from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
AAD 2016N
JHEP 1603 026 Search for Strong Gravity in Multijet Final States Produced in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV using the ATLAS Detector at the LHC
KHACHATRYAN 2016L
PRL 117 031802 Search for Narrow Resonances in Dijet Final States at $\sqrt {s }$ = 8 TeV with the Novel CMS Technique of Data Scouting
KHACHATRYAN 2016K
PRL 116 071801 Search for Narrow Resonances Decaying to Dijets in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
AAD 2013D
JHEP 1301 029 ATLAS Search for New Phenomena in Dijet Mass and Angular Distributions using ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AALTONEN 2013R
PRL 111 031802 Search for Pair-Production of Strongly-Interacting Particles Decaying to Pairs of Jets in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
CHATRCHYAN 2013A
JHEP 1301 013 Search for Narrow Resonances and Quantum Black Holes in Inclusive and ${\mathit {\mathit b}}$-Tagged Dijet Mass Spectra from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AAD 2012S
PL B708 37 Search for New Physics in the Dijet Mass Distribution using 1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 7 TeV Collected by the ATLAS Detector
CHATRCHYAN 2012BL
JHEP 1212 015 Search for Resonant ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production in Lepton+Jets Events in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AAD 2011AG
NJP 13 053044 A Search for New Physics in Dijet Mass and Angular Distributions in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV Measured with the ATLAS Detector
AALTONEN 2011M
PRL 106 171801 Invariant Mass Distribution of Jet Pairs Produced in Association with a ${{\mathit W}}$ Boson in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
ABAZOV 2011I
PRL 107 011804 Bounds on an Anomalous Dijet Resonance in ${{\mathit W}}$ +jets Production in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
AAD 2010
PRL 105 161801 Search for New Particles in Two-Jet Final States in 7 TeV Proton$−$Proton Collisions with the ATLAS Detector at the LHC
KHACHATRYAN 2010
PRL 105 211801 Search for Dijet Resonances in 7 TeV ${{\mathit p}}{{\mathit p}}$ Collisions at CMS
Also
PRL 106 029902 Publisher's Note to KHACHATRYAN 2010 : Search for Dijet Resonances in 7 TeV ${{\mathit p}}{{\mathit p}}$ Collisions at CMS
ABE 1999F
PRL 82 2038 Search for New Particles Decaying to ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ in ${{\mathit p}}$ ${{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV
ABE 1997G
PR D55 5263 Search for New Particles Decaying to Dijets at CDF
ABE 1993G
PRL 71 2542 Search for Quark Compositeness, Axigluons and Heavy Particles Using the Dijet Invariant Mass Spectrum Observed in ${{\mathit p}}$ ${{\overline{\mathit p}}}$ Collisions