cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.140841.v1/t3
title: "Table 2.2" of "Jet-like correlations with respect to K$^{0}_{\rm S}$ and $\Lambda$ ($\bar{\Lambda}$) in pp and Pb-Pb collisions at $\mathbf{\it\sqrt{s_\mathrm{NN}}}$ = 5.02 TeV"

description: Away-side of per-trigger yield modification, ($I_{\mathrm{AA}}$), of h$-$h, K$^{0}_\mathrm{S}-$h,and $(\Lambda+\overline{\Lambda})-$h trigger momentum range is $8&lt; p_{T}^{trig} &lt; 16~\mathrm{GeV}/c$, and associated charged particles momentum ranges which are showen in the table down.
description: Two-particle correlations with K$^{0}_\mathrm{S}$, $\Lambda/\overline{\Lambda}$, and charged hadrons as trigger particles in the transverse momentum range $8 &lt; p_\mathrm{T,trig}&lt;16$ GeV/$c$, and associated charged particles within $1 &lt; p_\mathrm{T,assoc}&lt;8$ GeV/$c$, are studied at mid-rapidity in pp and central Pb$-$Pb collisions at a centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector at the LHC.
After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb$-$Pb collisions with respect to pp collisions ($I_{\mathrm{AA}}$) is computed. The per-trigger yield in Pb$-$Pb collisions on the away side is strongly suppressed to the level of $I_{\mathrm{AA}}$
$\approx 0.6$ for $p_\mathrm{T,assoc}&gt;3$ GeV/$c$ as expected from strong in-medium energy loss, while an enhancement develops at low $p_\mathrm{T,assoc}$ on both the near and away sides, reaching $I_{\mathrm{AA}}$ $\approx 1.8$ and $2.7$ respectively. These findings are in good agreement with previous ALICE measurements from two-particle correlations triggered by neutral pions ($\pi^{0}$--h) and charged hadrons (h--h) in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}= 2.76$ TeV. Moreover, the correlations with K$^{0}_\mathrm{S}$ mesons and $\Lambda/\overline{\Lambda}$ baryons as trigger particles are compared to those of inclusive charged hadrons. The results are compared with the predictions of Monte Carlo models.
DOI: 10.17182/hepdata.140841.v1/t4
title: "Table 3.1" of "Jet-like correlations with respect to K$^{0}_{\rm S}$ and $\Lambda$ ($\bar{\Lambda}$) in pp and Pb-Pb collisions at $\mathbf{\it\sqrt{s_\mathrm{NN}}}$ = 5.02 TeV"

description: Near-side ratios of V^{0}-triggered yields to charged-hadron triggered (h$-$h) ones, ${{Y}^{K^{0}_{S}-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ and ${{Y}^{(\Lambda+\overline{\Lambda})-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ in Pb-Pb collisions.
description: Two-particle correlations with K$^{0}_\mathrm{S}$, $\Lambda/\overline{\Lambda}$, and charged hadrons as trigger particles in the transverse momentum range $8 &lt; p_\mathrm{T,trig}&lt;16$ GeV/$c$, and associated charged particles within $1 &lt; p_\mathrm{T,assoc}&lt;8$ GeV/$c$, are studied at mid-rapidity in pp and central Pb$-$Pb collisions at a centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector at the LHC.
After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb$-$Pb collisions with respect to pp collisions ($I_{\mathrm{AA}}$) is computed. The per-trigger yield in Pb$-$Pb collisions on the away side is strongly suppressed to the level of $I_{\mathrm{AA}}$
$\approx 0.6$ for $p_\mathrm{T,assoc}&gt;3$ GeV/$c$ as expected from strong in-medium energy loss, while an enhancement develops at low $p_\mathrm{T,assoc}$ on both the near and away sides, reaching $I_{\mathrm{AA}}$ $\approx 1.8$ and $2.7$ respectively. These findings are in good agreement with previous ALICE measurements from two-particle correlations triggered by neutral pions ($\pi^{0}$--h) and charged hadrons (h--h) in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}= 2.76$ TeV. Moreover, the correlations with K$^{0}_\mathrm{S}$ mesons and $\Lambda/\overline{\Lambda}$ baryons as trigger particles are compared to those of inclusive charged hadrons. The results are compared with the predictions of Monte Carlo models.
DOI: 10.17182/hepdata.140841.v1/t5
title: "Table 3.2" of "Jet-like correlations with respect to K$^{0}_{\rm S}$ and $\Lambda$ ($\bar{\Lambda}$) in pp and Pb-Pb collisions at $\mathbf{\it\sqrt{s_\mathrm{NN}}}$ = 5.02 TeV"

description: Away-side ratios of V^{0}-triggered yields to charged-hadron triggered (h$-$h) ones, ${{Y}^{K^{0}_{S}-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ and ${{Y}^{(\Lambda+\overline{\Lambda})-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ in Pb-Pb collisions.
description: Two-particle correlations with K$^{0}_\mathrm{S}$, $\Lambda/\overline{\Lambda}$, and charged hadrons as trigger particles in the transverse momentum range $8 &lt; p_\mathrm{T,trig}&lt;16$ GeV/$c$, and associated charged particles within $1 &lt; p_\mathrm{T,assoc}&lt;8$ GeV/$c$, are studied at mid-rapidity in pp and central Pb$-$Pb collisions at a centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector at the LHC.
After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb$-$Pb collisions with respect to pp collisions ($I_{\mathrm{AA}}$) is computed. The per-trigger yield in Pb$-$Pb collisions on the away side is strongly suppressed to the level of $I_{\mathrm{AA}}$
$\approx 0.6$ for $p_\mathrm{T,assoc}&gt;3$ GeV/$c$ as expected from strong in-medium energy loss, while an enhancement develops at low $p_\mathrm{T,assoc}$ on both the near and away sides, reaching $I_{\mathrm{AA}}$ $\approx 1.8$ and $2.7$ respectively. These findings are in good agreement with previous ALICE measurements from two-particle correlations triggered by neutral pions ($\pi^{0}$--h) and charged hadrons (h--h) in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}= 2.76$ TeV. Moreover, the correlations with K$^{0}_\mathrm{S}$ mesons and $\Lambda/\overline{\Lambda}$ baryons as trigger particles are compared to those of inclusive charged hadrons. The results are compared with the predictions of Monte Carlo models.
DOI: 10.17182/hepdata.140841.v1/t6
title: "Table 3.3" of "Jet-like correlations with respect to K$^{0}_{\rm S}$ and $\Lambda$ ($\bar{\Lambda}$) in pp and Pb-Pb collisions at $\mathbf{\it\sqrt{s_\mathrm{NN}}}$ = 5.02 TeV"

description: Near-side ratios of V^{0}-triggered yields to charged-hadron triggered (h--h) ones, ${{Y}^{K^{0}_{S}-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ and ${{Y}^{(\Lambda+\overline{\Lambda})-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ in pp collisions.
description: Two-particle correlations with K$^{0}_\mathrm{S}$, $\Lambda/\overline{\Lambda}$, and charged hadrons as trigger particles in the transverse momentum range $8 &lt; p_\mathrm{T,trig}&lt;16$ GeV/$c$, and associated charged particles within $1 &lt; p_\mathrm{T,assoc}&lt;8$ GeV/$c$, are studied at mid-rapidity in pp and central Pb$-$Pb collisions at a centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector at the LHC.
After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb$-$Pb collisions with respect to pp collisions ($I_{\mathrm{AA}}$) is computed. The per-trigger yield in Pb$-$Pb collisions on the away side is strongly suppressed to the level of $I_{\mathrm{AA}}$
$\approx 0.6$ for $p_\mathrm{T,assoc}&gt;3$ GeV/$c$ as expected from strong in-medium energy loss, while an enhancement develops at low $p_\mathrm{T,assoc}$ on both the near and away sides, reaching $I_{\mathrm{AA}}$ $\approx 1.8$ and $2.7$ respectively. These findings are in good agreement with previous ALICE measurements from two-particle correlations triggered by neutral pions ($\pi^{0}$--h) and charged hadrons (h--h) in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}= 2.76$ TeV. Moreover, the correlations with K$^{0}_\mathrm{S}$ mesons and $\Lambda/\overline{\Lambda}$ baryons as trigger particles are compared to those of inclusive charged hadrons. The results are compared with the predictions of Monte Carlo models.
DOI: 10.17182/hepdata.140841.v1/t7
title: "Table 3.4" of "Jet-like correlations with respect to K$^{0}_{\rm S}$ and $\Lambda$ ($\bar{\Lambda}$) in pp and Pb-Pb collisions at $\mathbf{\it\sqrt{s_\mathrm{NN}}}$ = 5.02 TeV"

description: Away-side ratios of V^{0}-triggered yields to charged-hadron triggered (h--h) ones, ${{Y}^{K^{0}_{S}-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ and ${{Y}^{(\Lambda+\overline{\Lambda})-\mathrm{h}}_{\Delta\varphi}}/{{Y}^{\mathrm{h-h}}_{\Delta\varphi}}$ in Pb-Pb collisions.
description: Two-particle correlations with K$^{0}_\mathrm{S}$, $\Lambda/\overline{\Lambda}$, and charged hadrons as trigger particles in the transverse momentum range $8 &lt; p_\mathrm{T,trig}&lt;16$ GeV/$c$, and associated charged particles within $1 &lt; p_\mathrm{T,assoc}&lt;8$ GeV/$c$, are studied at mid-rapidity in pp and central Pb$-$Pb collisions at a centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ALICE detector at the LHC.
After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb$-$Pb collisions with respect to pp collisions ($I_{\mathrm{AA}}$) is computed. The per-trigger yield in Pb$-$Pb collisions on the away side is strongly suppressed to the level of $I_{\mathrm{AA}}$
$\approx 0.6$ for $p_\mathrm{T,assoc}&gt;3$ GeV/$c$ as expected from strong in-medium energy loss, while an enhancement develops at low $p_\mathrm{T,assoc}$ on both the near and away sides, reaching $I_{\mathrm{AA}}$ $\approx 1.8$ and $2.7$ respectively. These findings are in good agreement with previous ALICE measurements from two-particle correlations triggered by neutral pions ($\pi^{0}$--h) and charged hadrons (h--h) in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}= 2.76$ TeV. Moreover, the correlations with K$^{0}_\mathrm{S}$ mesons and $\Lambda/\overline{\Lambda}$ baryons as trigger particles are compared to those of inclusive charged hadrons. The results are compared with the predictions of Monte Carlo models.
DOI: 10.17182/hepdata.140842.v1/t1
title: "Figure 1a-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: 1D correlation function. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t2
title: "Figure 1a-2" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^0(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t3
title: "Figure 1a-3" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^0(q)$ Fit. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t4
title: "Figure 1b-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^2_{x2}(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t5
title: "Figure 1b-2" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^2_{x2}(q)$ Fit. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t6
title: "Figure 1c-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^2_{y2}(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t7
title: "Figure 1c-2" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^2_{y2}(q)$ Fit. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t10
title: "Figure 1e-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^6_{y6}(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t11
title: "Figure 1e-2" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^6_{y6}(q)$ Fit. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t12
title: "Figure 1f-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^4_{x2y2}(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t13
title: "Figure 1f-2" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^4_{x2y2}(q)$ Fit. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t14
title: "Figure 1g-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^4_{x4}(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.
DOI: 10.17182/hepdata.140842.v1/t8
title: "Figure 1d-1" of "Source breakup dynamics in Au+Au Collisions at sqrt(s_NN)=200 GeV via three-dimensional two-pion source imaging"

description: Experimental correlation moments $R^6_{x6}(q)$ Data. Systematic errors are less than the statistical errors.
description: A three-dimensional (3D) correlation function obtained from mid-rapidity, low $p_T$ pion pairs in central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). Model comparisons to these distensions indicate a proper breakup time $\tau_0$ ~ 9 fm/$c$ and a mean proper emission duration $\Delta\tau$ ~ 2 fm/$c$, leading to sizable emission time differences ($&lt;|\Delta\tau_{LCM}|&gt;$ ~ 12 fm/$c$), partly due to resonance decays. They also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models.