LIMITS ON JET-JET RESONANCES

Heavy Particle Production Cross Section

INSPIRE   JSON  (beta) PDGID:
S015HP
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
HAYRAPETYAN
2024G
 CMS trijet resonance search
2
TUMASYAN
2023L
 CMS dijet resonance in 4-jet events
3
AAD
2020AD
 ATLS ${{\mathit p}}{{\mathit p}}$ at 13 TeV, dijet resonance
4
AAD
2020T
 ATLS dijet resonance search
5
AAD
2020W
 ATLS dijet resonance plus lepton
6
SIRUNYAN
2020AI
 CMS dijet resonance search
7
AABOUD
2019AJ
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit X}}$, ${{\mathit X}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
8
SIRUNYAN
2019B
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit A}}$, ${{\mathit A}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
9
SIRUNYAN
2019CD
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}{{\mathit \gamma}}$ , ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
10
AABOUD
2018AD
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Y}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ $\rightarrow$ ( ${{\mathit b}}{{\mathit b}}$) ${+}$ ( ${{\mathit q}}{{\mathit q}}$)
11
AABOUD
2018CK
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\mathit b}}{{\mathit b}}$ + $\not E_T$
12
AABOUD
2018CL
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ vector-like quarks
13
AABOUD
2018N
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
14
SIRUNYAN
2018DJ
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ or ${{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}{{\mathit j}}{{\mathit j}}$
15
SIRUNYAN
2018DY
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit R}}{{\mathit R}}$; ${{\mathit R}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
16
KHACHATRYAN
2017W
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
17
KHACHATRYAN
2017Y
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow(8 - 10$) ${{\mathit j}}+\not E_T$
18
SIRUNYAN
2017F
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ angular distribution
19
AABOUD
2016
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}$ + jet
20
AAD
2016N
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 3 high $\mathit E_{T}$ jets
21
AAD
2016S
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
22
KHACHATRYAN
2016K
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
23
KHACHATRYAN
2016L
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ resonance
24
AAD
2013D
 ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
25
AALTONEN
2013R
 CDF 1.96 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$4 jets
26
CHATRCHYAN
2013A
 CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
27
CHATRCHYAN
2013A
 CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit X}}$
28
AAD
2012S
 ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
29
CHATRCHYAN
2012BL
 CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit X}}$
30
AAD
2011AG
 ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$2 jets
31
AALTONEN
2011M
 CDF 1.96 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit W}}$+ 2 jets
32
ABAZOV
2011I
 D0 1.96 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit W}}$+ 2 jets
33
AAD
2010
ATLS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
34
KHACHATRYAN
2010
CMS 7 TeV ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ 2 jets
35
ABE
1999F
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$+ anything
36
ABE
1997G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
$ <2603 $ $95$ $200$ 37
ABE
1993G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
$ <44 $ $95$ $400$ 37
ABE
1993G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
$ <7 $ $95$ $600$ 37
ABE
1993G
 CDF 1.8 TeV ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ 2 jets
1  HAYRAPETYAN 2024G search for trijet resonance at CMS with 138 fb${}^{-1}$ of data at 13 TeV. No signal observed. Limits placed on various models vs mass(resonance).
2  TUMASYAN 2023L search for dijet resonance in 4-jet events with 138 fb${}^{-1}$ fb of data. There are two events in the tails of the distributions, each with a four-jet mass of 8 TeV and an average dijet mass of 2 TeV, resulting in local and global significances of 3.9 and 1.6 standard deviations, respectively, if interpreted as a signal. Limits set for simplified diquark model.
3  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.
4  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.
5  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.
6  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.
7  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.
8  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.
9  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.
10  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.
11  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.
12  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.
13  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.
14  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.
15  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.
16  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.
17  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.
18  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.
19  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.
20  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).
21  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.
22  KHACHATRYAN 2016K search for dijet resonance in 2.4 fb${}^{-1}$ data at 13 TeV; see Fig. 3 for limits on axigluons, diquarks etc.
23  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.
24  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.
25  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.
26  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.
27  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.
28  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.
29  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.
30  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.
31  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${}^{-1}$.
32  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.
33  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.
34  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 ${{\mathit g}}{{\mathit g}}$.
35  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.
36  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 $10^{4} - 10^{-1}~$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.
37  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