cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.159918.v1/t12
title: "Acceptance ($A$) and efficiency ($\varepsilon$)" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The product of acceptance, $A$, and efficiency, $\varepsilon$, of a resonant signal with $\alpha_{\mathrm{true}}$ = 0.25 vs. the diquark mass for various diquark widths, and for all $\alpha$ bins inclusively. The acceptance is defined as the fraction of generated events passing the kinematic selection criteria, while the efficiency is the fraction of signal events satisfying $m_{\mathrm{4j}} &gt; 1.6$ TeV. We also show the signal acceptance alone in the curves where $\varepsilon = 1$.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t13
title: "Four-jet mass spectra for 0.22 &lt; $\alpha$ &lt; 0.24" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The four-jet mass distribution in data for 0.22 &lt; $\alpha$ &lt; 0.24, fitted with three background-only functions (Dijet-3p, PowExp-3p and ModDijet-3p), each with three free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV, and $\Gamma/M_{\mathrm{S}}$ = 1.5%, 10% are also shown, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t14
title: "Four-jet mass spectra for 0.24 &lt; $\alpha$ &lt; 0.26" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The four-jet mass distribution in data for 0.24 &lt; $\alpha$ &lt; 0.26, fitted with three background-only functions (Dijet-3p, PowExp-3p and ModDijet-3p), each with three free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV, and $\Gamma/M_{\mathrm{S}}$ = 1.5%, 10% are also shown, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t15
title: "Four-jet mass spectra for 0.26 &lt; $\alpha$ &lt; 0.28" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The four-jet mass distribution in data for 0.26 &lt; $\alpha$ &lt; 0.28, fitted with three background-only functions (Dijet-3p, PowExp-3p and ModDijet-3p), each with three free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV and $\alpha_{\mathrm{true}}$ = 0.29, $M_{\mathrm{S}}$ = 3.6 TeV, each shown for widths of $\Gamma/M_{\mathrm{S}}$ = 1.5% and 10% are also included, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t16
title: "Four-jet mass spectra for 0.28 &lt; $\alpha$ &lt; 0.30" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The four-jet mass distribution in data for 0.28 &lt; $\alpha$ &lt; 0.30, fitted with three background-only functions (Dijet-3p, PowExp-3p and ModDijet-3p), each with three free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV and $\alpha_{\mathrm{true}}$ = 0.29, $M_{\mathrm{S}}$ = 3.6 TeV, each shown for widths of $\Gamma/M_{\mathrm{S}}$ = 1.5% and 10% are also included, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t17
title: "Four-jet mass spectra for 0.30 &lt; $\alpha$ &lt; 0.32" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The four-jet mass distribution in data for 0.30 &lt; $\alpha$ &lt; 0.32, fitted with three background-only functions (Dijet-3p, PowExp-3p and ModDijet-3p), each with three free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV and $\alpha_{\mathrm{true}}$ = 0.29, $M_{\mathrm{S}}$ = 3.6 TeV, each shown for widths of $\Gamma/M_{\mathrm{S}}$ = 1.5% and 10% are also included, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t9
title: "$m_{4j}$ vs. $\alpha$ contour (5% width)" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 68% probability contour in the $m_{\mathrm{4j}}$ vs. $\alpha$ plane from a signal simulation of a diquark with a width of 5% and a mass of 8.4 TeV, decaying to a pair of vector-like quarks, each with a mass of 2.1 TeV.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t18
title: "Four-jet mass spectra for 0.32 &lt; $\alpha$ &lt; 0.34" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The four-jet mass distribution in data for 0.32 &lt; $\alpha$ &lt; 0.34, fitted with three background-only functions (Dijet-3p, PowExp-3p and ModDijet-3p), each with three free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV, and $\Gamma/M_{\mathrm{S}}$ = 1.5%, 10% are also shown, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t19
title: "Inclusive four-jet mass spectra for $\alpha$ &gt; 0.10" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The inclusive four-jet mass distribution in data for $\alpha$ &gt; 0.10, fitted with three background-only functions (Dijet-5p, PowExp-5p and ModDijet-5p), each with five free parameters. Examples of predicted diquark resonances with $\alpha_{\mathrm{true}}$ = 0.25, $M_{\mathrm{S}}$ = 8.6 TeV and $\alpha_{\mathrm{true}}$ = 0.29, $M_{\mathrm{S}}$ = 3.6 TeV, each shown for widths of $\Gamma/M_{\mathrm{S}}$ = 1.5% and 10% are also included, with cross sections equal to the observed upper limits at 95% confidence level.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.