cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.151167.v1/t21
title: "Figure 26b" 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.
DOI: 10.17182/hepdata.151167.v1/t22
title: "Figure 27" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Near-side and far-side $p_{out}$ distributions for minimum bias $d$+Au collisions obtained from $\pi^{\pm}$ - $h^{\pm}$ correlation. The trigger is 5 &lt; $p_{T,trig}$ &lt; 10 GeV/$c$, the associated particle is 0.5 &lt; $p_{T,assoc}$ &lt; 5.0 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/t23
title: "Figure 28a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Conditional yield as a function of $x_E$ for near-side and far-side for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ 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/t24
title: "Figure 28b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Conditional yield as a function of $x_E$ for near-side and far-side for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ 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/t25
title: "Figure 29" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Conditional yield as a function of $x_E$ for near-side and far-side correlations for $\pi^{\pm}$ - $h^{\pm}$ correlations from minimum-bias $d$+Au collisions. The trigger pions are 5 &lt; $p_{T,trig}$ &lt; 6 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/t26
title: "Figure 30" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Conditional yield as a function of $x_E$ for near-side and far-side correlation for $\pi^{\pm}$ - $h^{\pm}$ correlation for several different trigger $p_T$s for 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/t27
title: "Figure 32a" 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 $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for 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/t28
title: "Figure 32b" 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 $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for 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/t29
title: "Figure 32c" 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 $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for 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/t30
title: "Figure 32d" 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 $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for 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/t31
title: "Figure 33a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The comparison of the $\sqrt{}$ values between $d$+Au and $p$+$p$ for the $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations. The trigger pion range is 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/t32
title: "Figure 33b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The comparison of the $\sqrt{}$ values between $d$+Au and $p$+$p$ for the $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations. The trigger pion range is 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/t33
title: "Figure 35a" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Quadrature difference between minimum-bias $d$+Au and $p$+$p$ $$ values.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, 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/t34
title: "Figure 35b" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Quadrature difference between minimum-bias $d$+Au and $p$+$p$ $$ values.
description: BNL-RHIC. Dihadron correlations at high transverse momentum in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at midrapidity are measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). From these correlations we extract several structural characteristics of jets; the root-mean-squared (RMS) transverse momentum of fragmenting hadrons with respect to the jet $\sqrt{}$, the mean sine-squared angle between the scattered partons $$, 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/t35
title: "Figure 36" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The comparison of the $p_{out}$ distribution at the near-side and far-side between central $d$+Au collisions and $p$+$p$ collisions. Results are obtained for $\pi^{\pm}$ - $h^{\pm}$ correlations with the associated hadron range 0.5 &lt; $p_{T,assoc}$ &lt; 5 GeV/$c$ and trigger pion range of 5 &lt; $p_{T,trig}$ &lt; 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/t36
title: "Figure 37" of "Jet structure from dihadron correlations in d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The comparison of the $x_E$ distribution from $\pi^{\pm}$ - $h^{\pm}$ correlation at the near-side and far-side between minimum bias $d$+Au collisions and $p$+$p$ collisions. The trigger $\pi^{\pm}$ are 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.