cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.151167.v1/t37
title: "Figure 38a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t38
title: "Figure 38b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t39
title: "Figure 38c" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t40
title: "Figure 39" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The fitted fractional change in $dN/d_{x_E}$ per unit $p_{T,trig}$ of the far-side conditional yield for different ranges of $x_E$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t41
title: "Figure 41a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Centrality dependent near and far $CY(p_T)$ for $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t42
title: "Figure 41b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Centrality dependent near and far $CY(p_T)$ for $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t43
title: "Figure 42a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Centrality dependence to the ratio of near and far $CY(p_T)$ for $d$+Au to $p$+$p$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t44
title: "Figure 42b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Centrality dependence to the ratio of near and far $CY(p_T)$ for $d$+Au to $p$+$p$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t45
title: "Table XI" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side widths as a function of $p_{T, trig}$ for charged pion triggers and associated charged hadrons (2–4.5 Gev/$c$) from minimum-bias $d$+Au collisions.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151167.v1/t46
title: "Table XII" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side widths as a function of $p_{T, trig}$ for neutral pion triggers and associated charged hadrons (2–4.5 Gev/$c$) from minimum-bias $d$+Au collisions.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, and the number of particles produced within the dijet that are associated with a high-$p_T$ particle ($dN/dx_E$ distributions). We observe that the fragmentation characteristics of jets in $d$+Au collisions are very similar to those in $p$+$p$ collisions and that there is also little dependence on the centrality of the $d$+Au collision. This is consistent with the nuclear medium having little influence on the fragmentation process. Furthermore, there is no statistically significant increase in the value of $$ from $p$+$p$ to $d$+Au collisions. This constrains the amount of multiple scattering that partons undergo in the cold nuclear medium before and after a hard-collision.
DOI: 10.17182/hepdata.151276.v1/t1
title: " 95% CL upper limits on $\mu_{HH}$ (obs and exp)" of "Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the $b\bar{b}\tau^+\tau^-$ final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Observed (filled circles) and expected (open circles) 95% CL upper limits on $\mu_{HH}$ from the fit of each individual channel and the combined fit in the background-only ($\mu_{HH} = 0$) hypothesis. The dashed lines indicate the expected 95% CL upper limits on $\mu_{HH}$ in the SM hypothesis ($\mu_{HH} = 1$). The inner and outer bands indicate the $\pm 1\sigma$ and $\pm 2\sigma$ variations, respectively, on the expected limit with respect to the background-only hypothesis due to statistical and systematic uncertainties.
description: A search for non-resonant production of Higgs boson pairs in the $HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ channel is performed using 140 $\mathrm{fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. The analysis strategy is optimised to probe anomalous values of the Higgs boson self-coupling modifier $\kappa_{\lambda}$ and of the quartic $HHVV$ ($V = W, Z$) coupling modifier $\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed (expected) upper limit $\mu_{HH} &lt; 5.9 (3.3)$ is set at 95% confidence-level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The coupling modifiers are constrained to an observed (expected) 95% confidence interval of $-3.1 &lt; \kappa_{\lambda} &lt; 9.0$ $(-2.5 &lt; \kappa_{\lambda} &lt; 9.3)$ and $-0.5 &lt; \kappa_{2V} &lt; 2.7$ $(-0.2 &lt; \kappa_{2V} &lt; 2.4)$, assuming all other Higgs boson couplings are fixed to the Standard Model prediction. The results are also interpreted in the context of effective field theories via constraints on anomalous Higgs boson couplings and Higgs boson pair production cross-sections assuming different kinematic benchmark scenarios.
DOI: 10.17182/hepdata.151276.v1/t2
title: "Upper limits on ggF, VBF and HH $\mu$ (obs and exp)" of "Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the $b\bar{b}\tau^+\tau^-$ final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Observed and expected 95% CL upper limits on $\mu_{HH}$, $\mu_{ggF}$ and $\mu_{VBF}$ from the individual SR likelihood fits as well as the combined results. The $\mu_{ggF}$ and $\mu_{VBF}$ limits are quoted both from the results of the simultaneous fit of both signal strengths (central column), and from independent fits for the individual production modes, assuming the other to be as predicted by the SM. The uncertainties quoted on the combined expected upper limits correspond to the 1σ uncertainty band.
description: A search for non-resonant production of Higgs boson pairs in the $HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ channel is performed using 140 $\mathrm{fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. The analysis strategy is optimised to probe anomalous values of the Higgs boson self-coupling modifier $\kappa_{\lambda}$ and of the quartic $HHVV$ ($V = W, Z$) coupling modifier $\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed (expected) upper limit $\mu_{HH} &lt; 5.9 (3.3)$ is set at 95% confidence-level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The coupling modifiers are constrained to an observed (expected) 95% confidence interval of $-3.1 &lt; \kappa_{\lambda} &lt; 9.0$ $(-2.5 &lt; \kappa_{\lambda} &lt; 9.3)$ and $-0.5 &lt; \kappa_{2V} &lt; 2.7$ $(-0.2 &lt; \kappa_{2V} &lt; 2.4)$, assuming all other Higgs boson couplings are fixed to the Standard Model prediction. The results are also interpreted in the context of effective field theories via constraints on anomalous Higgs boson couplings and Higgs boson pair production cross-sections assuming different kinematic benchmark scenarios.
DOI: 10.17182/hepdata.151276.v1/t3
title: "Combined $-2\ln\Lambda$ vs $\kappa_{\lambda}$ obs" of "Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the $b\bar{b}\tau^+\tau^-$ final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Observed (solid line) value of $-2\ln\Lambda$ as a function of $\kappa_{\lambda}$ for the combined fit, when all other coupling modifiers are fixed to their SM predictions.
description: A search for non-resonant production of Higgs boson pairs in the $HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ channel is performed using 140 $\mathrm{fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. The analysis strategy is optimised to probe anomalous values of the Higgs boson self-coupling modifier $\kappa_{\lambda}$ and of the quartic $HHVV$ ($V = W, Z$) coupling modifier $\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed (expected) upper limit $\mu_{HH} &lt; 5.9 (3.3)$ is set at 95% confidence-level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The coupling modifiers are constrained to an observed (expected) 95% confidence interval of $-3.1 &lt; \kappa_{\lambda} &lt; 9.0$ $(-2.5 &lt; \kappa_{\lambda} &lt; 9.3)$ and $-0.5 &lt; \kappa_{2V} &lt; 2.7$ $(-0.2 &lt; \kappa_{2V} &lt; 2.4)$, assuming all other Higgs boson couplings are fixed to the Standard Model prediction. The results are also interpreted in the context of effective field theories via constraints on anomalous Higgs boson couplings and Higgs boson pair production cross-sections assuming different kinematic benchmark scenarios.
DOI: 10.17182/hepdata.151276.v1/t4
title: "Combined $-2\ln\Lambda$ vs $\kappa_{\lambda}$ exp" of "Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the $b\bar{b}\tau^+\tau^-$ final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Expected (dashed line) value of $-2\ln\Lambda$ as a function of $\kappa_{\lambda}$ for the combined fit, when all other coupling modifiers are fixed to their SM predictions.
description: A search for non-resonant production of Higgs boson pairs in the $HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ channel is performed using 140 $\mathrm{fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. The analysis strategy is optimised to probe anomalous values of the Higgs boson self-coupling modifier $\kappa_{\lambda}$ and of the quartic $HHVV$ ($V = W, Z$) coupling modifier $\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed (expected) upper limit $\mu_{HH} &lt; 5.9 (3.3)$ is set at 95% confidence-level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The coupling modifiers are constrained to an observed (expected) 95% confidence interval of $-3.1 &lt; \kappa_{\lambda} &lt; 9.0$ $(-2.5 &lt; \kappa_{\lambda} &lt; 9.3)$ and $-0.5 &lt; \kappa_{2V} &lt; 2.7$ $(-0.2 &lt; \kappa_{2V} &lt; 2.4)$, assuming all other Higgs boson couplings are fixed to the Standard Model prediction. The results are also interpreted in the context of effective field theories via constraints on anomalous Higgs boson couplings and Higgs boson pair production cross-sections assuming different kinematic benchmark scenarios.