cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.159889.v1/t9
title: "Figure 6 EPOS" of "Measurement of the transverse energy density in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV with the sPHENIX detector"

description: Measured $\frac{dE_T}{d\eta}$ normalized by the estimated number of participant pairs ($0.5$$N_{part}$), as a function of $N_{part}$, predictions from EPOS.
description: BNL-RHIC. This paper reports measurements of the transverse energy per unit pseudorapidity ($dE_{T}/d\eta$) produced in $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV, performed with the sPHENIX detector at the Relativistic Heavy Ion Collider (RHIC). The results cover the pseudorapidity range $\left|\eta\right| &lt; 1.1$ and constitute the first such measurement performed using a hadronic calorimeter at RHIC. Measurements of $dE_{T}/d\eta$ are presented for a range of centrality intervals and the average $dE_{T}/d\eta$ as a function of the number of participating nucleons, $N_{part}$, is compared to a variety of Monte Carlo heavy-ion event generators. The results are in agreement with previous measurements at RHIC, and feature an improved granularity in $\eta$ and improved precision in low-$N_{part}$ events.
DOI: 10.17182/hepdata.159918.v1/t1
title: "2D $m_{4\mathrm{j}}$ vs. $\overline{m}_{\mathrm{2j}}$ for data" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed number of events within bins of the four-jet mass and the average mass of the two dijets.
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/t2
title: "2D $m_{\mathrm{4j}}$ vs. $\alpha$ for data" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed number of events within bins of the four-jet mass and the ratio $\alpha$, which is the average dijet mass divided by the four-jet mass.
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/t4
title: "2D $m_{4\mathrm{j}}$ vs. $\alpha$ for QCD MC" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predictions of a leading order (LO) QCD simulation, normalized to an integrated luminosity of 138 fb$^{-1}$. The number of events are examined within bins of the four-jet mass and the ratio $\alpha$, which is the average dijet mass divided by the four-jet mass.
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/t3
title: "2D $m_{4\mathrm{j}}$ vs. $\overline{m}_{\mathrm{2j}}$ for QCD MC" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predictions of a leading order (LO) QCD simulation, normalized to an integrated luminosity of 138 fb$^{-1}$. The number of events are examined within bins of the four-jet mass and the average mass of the two dijets.
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/t5
title: "$m_{4j}$ vs. $\overline{m}_{2j}$ contour (1.5% 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. $\overline{m}_{\mathrm{2j}}$ plane from a signal simulation of a diquark with a width of 1.5% 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/t6
title: "$m_{4j}$ vs. $\overline{m}_{2j}$ 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. $\overline{m}_{\mathrm{2j}}$ 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/t7
title: "$m_{4j}$ vs. $\overline{m}_{2j}$ contour (10% 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. $\overline{m}_{\mathrm{2j}}$ plane from a signal simulation of a diquark with a width of 10% 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/t8
title: "$m_{4j}$ vs. $\alpha$ contour (1.5% 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 1.5% 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: 10.15472/sq7sba
title: Hongos fitopatógenos del género Fusarium en frutales

description: Hongos fitopatógenos del género Fusarium spp. aislados de raíz y cuello de plantas de Physalis peruviana (uchuva), procedentes de cultivos comerciales en los departamentos de Antioquia, Boyacá y Cundinamarca
DOI: 10.17182/hepdata.159918.v1/t10
title: "$m_{4j}$ vs. $\alpha$ contour (10% 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 10% 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/t11
title: "Signal shapes" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal differential distributions as a function of four-jet mass for $\alpha_{\mathrm{true}}$ = 0.25, diquark masses of 2, 5, 8.6 TeV and various widths, for all $\alpha$ bins inclusively. The integral of each distribution has been normalized to unity.
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.