cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.102318.v1/t5
title: "Figure 3.0" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of charged particles as a function of $p_T$ for minimum bias Au+Au collisions at 130 GeV.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102318.v1/t6
title: "Figure 3.1" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of $K_s^0$ as a function of $p_T$ for minimum bias Au+Au collisions at 130 GeV. Systematic errors of $\pm$0.005 for particle identification and background subtraction and $^{+0}_{-0.005}$ for nonflow effects.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102318.v1/t7
title: "Figure 3.2" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of $\Lambda+\bar{\Lambda}$ as a function of $p_T$ for minimum bias Au+Au collisions at 130 GeV. Systematic errors of $\pm$0.005 for particle identification and background subtraction and $^{+0}_{-0.005}$ for nonflow effects.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102318.v1/t8
title: "Figure 4.0" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $p_T$-integrated $v_2$ of $h^-$, $K_s^0$, and $\Lambda+\bar{\Lambda}$ as a function of particle mass for minimum bias Au+Au collisions at 130 GeV.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102319.v1/t1
title: "Figure 3.0" of "Coherent rho0 production in ultra-peripheral heavy ion collisions."

description: Differential cross section $d\sigma(\gamma Au \rightarrow \rho Au)/dt$ of $\rho^0$ candidates
description: The STAR Collaboration reports the first observation of exclusive $\rho^0$ photoproduction, $AuAu\rightarrow AuAu\rho^0$, and $\rho^0$ production accompanied by mutual nuclear Coulomb excitation, $AuAu\rightarrow Au^\ast Au^\ast \rho^0$, in ultraperipheral heavy-ion collisions. The $\rho^0$ have low transverse momenta, consistent with coherent coupling to both nuclei. The cross sections at $\sqrt{s_{_{NN}}}$ = 130 GeV agree with theoretical predictions treating $\rho^0$ production and Coulomb excitation as independent processes.
DOI: 10.17182/hepdata.102319.v1/t2
title: "Figure 4.0" of "Coherent rho0 production in ultra-peripheral heavy ion collisions."

description: Differential cross section $d\sigma/dM_{\pi\pi}$ for two-track (xn,xn) events with pair $p_T&lt;150$ MeV/$c$
description: The STAR Collaboration reports the first observation of exclusive $\rho^0$ photoproduction, $AuAu\rightarrow AuAu\rho^0$, and $\rho^0$ production accompanied by mutual nuclear Coulomb excitation, $AuAu\rightarrow Au^\ast Au^\ast \rho^0$, in ultraperipheral heavy-ion collisions. The $\rho^0$ have low transverse momenta, consistent with coherent coupling to both nuclei. The cross sections at $\sqrt{s_{_{NN}}}$ = 130 GeV agree with theoretical predictions treating $\rho^0$ production and Coulomb excitation as independent processes.
DOI: 10.17182/hepdata.102319.v1/t3
title: "Figure 4.1" of "Coherent rho0 production in ultra-peripheral heavy ion collisions."

description: Total background in the differential cross section $d\sigma/dM_{\pi\pi}$
description: The STAR Collaboration reports the first observation of exclusive $\rho^0$ photoproduction, $AuAu\rightarrow AuAu\rho^0$, and $\rho^0$ production accompanied by mutual nuclear Coulomb excitation, $AuAu\rightarrow Au^\ast Au^\ast \rho^0$, in ultraperipheral heavy-ion collisions. The $\rho^0$ have low transverse momenta, consistent with coherent coupling to both nuclei. The cross sections at $\sqrt{s_{_{NN}}}$ = 130 GeV agree with theoretical predictions treating $\rho^0$ production and Coulomb excitation as independent processes.
DOI: 10.17182/hepdata.102320.v1/t1
title: "Figure 1.0" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: $p$ differential yield. Systematic uncertainties are $\pm$10%.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t2
title: "Figure 1.1" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: $\bar{p}$ differential yield. Systematic uncertainties are $\pm$10%.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t4
title: "Figure 2.1" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: Rapidity distribution of $\bar{p}$. Combined statitiscal uncertainty and systematic uncertainty from PID contramination. Systematic uncertainties from the track reconstruction efficiency are $\pm$25%.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t5
title: "Figure 2.2" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: Average transverse momentum of $p+\bar{p}$. Systematic uncertainties are $\pm$6%.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t11
title: "Figure 3.5" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: $dN/dy$ vs. the number of negative hadrons. Systematic error bands in figure are $\pm$25% for dN/dy.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t3
title: "Figure 2.0" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: Rapidity distribution of $p$. Combined statitiscal uncertainty and systematic uncertainty from PID contramination. Systematic uncertainties from the track reconstruction efficiency are $\pm$25%.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t6
title: "Figure 3.0" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: Average transverse momentum vs. centrality. Systematic error bands in figure are $\pm$6% for .
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t8
title: "Figure 3.2" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: $dN/dy$ vs. centrality. Systematic error bands in figure are $\pm$25% for dN/dy.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t9
title: "Figure 3.3" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: Average transverse momentum vs. the number of negative hadrons. Systematic error bands in figure are $\pm$6% for .
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t10
title: "Figure 3.4" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: $dN/dy$ vs. the number of negative hadrons. Systematic error bands in figure are $\pm$25% for dN/dy.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102320.v1/t7
title: "Figure 3.1" of "Rapidity and centrality dependence of proton and anti-proton production from Au-197 + Au-197 collisions at s(NN)**(1/2) = 130-GeV."

description: $dN/dy$ vs. centrality. Systematic error bands in figure are $\pm$25% for dN/dy.
description: We report on the rapidity and centrality dependence of proton and antiproton transverse mass distributions from Au+Au collisions at 130 GeV as measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). Our results are from the rapidity and transverse momentum range of $|y|&lt;0.5$ and $0.35
DOI: 10.17182/hepdata.102321.v1/t1
title: "Figure 1.0" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: $m_T$ spectra of $\Xi^-$ and $\bar{\Xi}^+$ for 0-10% centrality. Errors listed here are the quadrature sum of statistical and point-to-point systematic uncertainties. There is an additional overall $m_T$-independent systematic uncertainty of 10%.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t2
title: "Figure 1.1" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: $m_T$ spectra of $\Xi^-$ and $\bar{\Xi}^+$ for 10-25% centrality. Errors listed here are the quadrature sum of statistical and point-to-point systematic uncertainties. There is an additional overall $m_T$-independent systematic uncertainty of 10%.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t3
title: "Figure 1.2" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: $m_T$ spectra of $\Xi^-$ and $\bar{\Xi}^+$ for 25-75% centrality. Errors listed here are the quadrature sum of statistical and point-to-point systematic uncertainties. There is an additional overall $m_T$-independent systematic uncertainty of 10%.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t4
title: "Figure 1.3" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: $m_T$ spectra of $\Omega^-+\bar{\Omega}^+$ for 0-10% centrality. Errors listed here are the quadrature sum of statistical and point-to-point systematic uncertainties. There is an additional overall $m_T$-independent systematic uncertainty of 10%.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t10
title: "Table 2.1" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Particle ratio from nonequilibrium model.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t11
title: "Table 2.2" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Particle ratio from HIJING/$B\bar{B}$.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t5
title: "Table 1.0" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Fit parameters for $m_T$ spectra of $\Xi^-$.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t6
title: "Table 1.1" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Fit parameters for $m_T$ spectra of $\bar{\Xi}^+$.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t7
title: "Table 1.2" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Fit parameters for $m_T$ spectra of $\Omega^-+\bar{\Omega}^+$.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t8
title: "Figure 2.0" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Particle ratio in 0-10% centrality.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t9
title: "Table 2.0" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Particle ratio in 0-10% centrality from the statiscal model.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.