cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.151167.v1/t4
title: "Figure 14" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Fully corrected assorted $\pi^{0}$-hadron conditional pair distributions for $d$+Au collisions centrality 0-88% and $p$+$p$ collisions. The trigger $\pi^0$s are within 5 &lt; $p_{T,trig}$ &lt; 10 GeV/$c$ and are correlated with hadrons with $p_{T,assoc}$ of 1.5-2 GeV/$c$, 2-3GeV/$c$, 3-4 GeV/$c$, and 4-5 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/t6
title: "Figure 16a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near-side width, far-side width as a function of $p_{T,assoc}$ for a charged pion and neutral pion triggers from the $p_{T,trig}$ range of 5-10 GeV/$c$ in 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/t7
title: "Figure 16b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near-side width, far-side width as a function of $p_{T,assoc}$ for a charged pion and neutral pion triggers from the $p_{T,trig}$ range of 5-10 GeV/$c$ in 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/t8
title: "Figure 20a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged hadron triggers (2.5−4 GeV/$c$) and associated charged hadrons from $d$+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/t9
title: "Figure 20b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged hadron triggers (4−6 GeV/$c$) and associated charged hadrons from $d$+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/t11
title: "Figure 21b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side conditional yields as a function of $p_{T, assoc}$ for neutral pion triggers (5−10 GeV/$c$) and associated charged hadrons 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/t12
title: "Figure 22" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side widths and conditional yields as a function of $N_{coll}$ for charged hadron triggers (2.5−4 GeV/$c$) and associated charged hadrons (1–2.5 GeV/$c$) from $d$+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/t13
title: "Figure 23" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near- and far-side widths and conditional yields as a function of centrality for neutral pion triggers (5−10 GeV/$c$) and associated charged hadrons (2–3 GeV/$c$) from $d$+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/t14
title: "Figure 24a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The extracted $\sqrt{}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ 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/t15
title: "Figure 24b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The extracted $\sqrt{}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ 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/t16
title: "Figure 24c" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The extracted $\sqrt{}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ 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/t17
title: "Figure 24d" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The extracted $\sqrt{}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ 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/t18
title: "Figure 25a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $$ for minimum bias $d$+Au collisions as function of associated particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations where the trigger particles have a $p_T$ between 5 - 10 GeV/$c$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, 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/t19
title: "Figure 25b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $$ for minimum bias $d$+Au collisions as function of associated particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations where the trigger particles have a $p_T$ between 5 - 10 GeV/$c$.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, 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/t20
title: "Figure 26a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $$ for minimum bias $d$+Au collisions as function of trigger particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, 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.