cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.142287.v1/t9
title: "Figure 11b" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t11
title: "Figure 13" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The near and away side conditional yield per number of triggers for 1.4 &lt; $p_{Ta}$ &lt; 5.0 GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t12
title: "Figure 14a" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t13
title: "Figure 14b" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t14
title: "Figure 14c" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t15
title: "Figure 15" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t16
title: "Figures 18a" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t17
title: "Figures 18b" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t18
title: "Figures 18c" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t19
title: "Figures 18d" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t20
title: "Figures 18e" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t21
title: "Figure 22" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Extracted values of $D(x)$ parameters according from the fit to the LEP data and power $n$ of the unmeasured final state parton spectra $\Sigma_q(\bar{p_T})$ extracted from the fit to the single inclusive $\pi^0$ invariant cross section for corresponding fragmentation and fixed values of $\sqrt{}$ = 2.5 GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t22
title: "Figures 16a & 26a" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\bar{x^-1_h}$ $$ $\sqrt{}$ $\sqrt{}$ values as a function of $p_{Ta}$ for two different trigger $\pi^0$ transverse momentum bins.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t23
title: "Figures 16b & 26b" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\bar{x^-1_h}$ $$ $\sqrt{}$ $\sqrt{}$ values as a function of $p_{Ta}$ for two different trigger $\pi^0$ transverse momentum bins.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t24
title: "Figures 17 & 27" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Values of $\bar{x^-1_h}$ $$ $\sqrt{}$ and $\sqrt{}$ for various trigger particle $p_{Tt}$ and associated momenta in 1.4 &lt; $p_{Ta}$ &lt; 5.0 GeV/$c$ region.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t25
title: "Figure 28" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $$ and $\bar{x_h}$ values with $p_{Tt}$
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.