cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.134956.v1/t27
title: "Table 27" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV (Multiplicity class 40-60%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t28
title: "Table 28" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV (Multiplicity class 60-80%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t29
title: "Table 29" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV (Multiplicity class 0-10%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t30
title: "Table 30" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV (Multiplicity class 10-20%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t31
title: "Table 31" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV (Multiplicity class 20-30%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t32
title: "Table 32" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV (Multiplicity class 30-40%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t33
title: "Table 33" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV (Multiplicity class 40-60%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t34
title: "Table 34" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$-differential yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV (Multiplicity class 60-80%).
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t35
title: "Table 35" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$- integrated yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$7.7 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t36
title: "Table 36" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$- integrated yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$11.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t37
title: "Table 37" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$- integrated yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$14.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t39
title: "Table 39" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$- integrated yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t38
title: "Table 38" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$- integrated yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$19.6 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t40
title: "Table 40" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $p_{\mathrm T}$- integrated yield of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t41
title: "Table 41" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: &lt;$p_{\mathrm T}$&gt; of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$7.7 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t42
title: "Table 42" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: &lt;$p_{\mathrm T}$&gt; of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$11.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t43
title: "Table 43" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: &lt;$p_{\mathrm T}$&gt; of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$14.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t44
title: "Table 44" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: &lt;$p_{\mathrm T}$&gt; of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$19.6 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t45
title: "Table 45" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: &lt;$p_{\mathrm T}$&gt; of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t46
title: "Table 46" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: &lt;$p_{\mathrm T}$&gt; of $\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t47
title: "Table 47" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$7.7 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t48
title: "Table 48" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$11.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t49
title: "Table 49" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$14.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t50
title: "Table 50" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$19.6 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t51
title: "Table 51" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t52
title: "Table 52" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t53
title: "Table 53" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. $&lt;(dN_{ch}/dy)^{1/3}&gt;$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$7.7 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t54
title: "Table 54" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. $&lt;(dN_{ch}/dy)^{1/3}&gt;$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~11.5 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t55
title: "Table 55" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. $&lt;(dN_{ch}/dy)^{1/3}&gt;$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$14.5GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t56
title: "Table 56" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. $&lt;(dN_{ch}/dy)^{1/3}&gt;$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$19.6 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t57
title: "Table 57" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. $&lt;(dN_{ch}/dy)^{1/3}&gt;$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t58
title: "Table 58" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{\mathrm{K^{*0}} + \bar{\mathrm{K^{*0}}}}{K^{+} + K^{-}}$ vs. $&lt;(dN_{ch}/dy)^{1/3}&gt;$ in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV. Total systematic error is the quadrature sum of the correlated and uncorrelated systematic errors
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t59
title: "Table 59" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{2\phi}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$7.7 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t60
title: "Table 60" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{2\phi}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$11.5 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t61
title: "Table 61" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{2\phi}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$19.6 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t62
title: "Table 62" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{2\phi}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t63
title: "Table 63" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: $\frac{2\phi}{K^{+} + K^{-}}$ vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t64
title: "Table 64" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$7.7 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t65
title: "Table 65" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$11.5 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t66
title: "Table 66" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$14.5 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t67
title: "Table 67" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$19.6 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t68
title: "Table 68" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$27 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t69
title: "Table 69" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$39 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t70
title: "Table 70" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$62.4 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.134956.v1/t71
title: "Table 71" of "$K^{*0}$ production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan"

description: lower limit of hadronic phase lifetime vs. &lt; Npart &gt; in AuAu collisions at $\sqrt{s_{\mathrm{NN}}}~=~$200 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.135073.v1/t1
title: "Data TEEC" of "Determination of the strong coupling constant from transverse energy$-$energy correlations in multijet events at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Particle-level TEEC results
description: CERN-LHC. Asymptotic freedom beyond the TeV scale and determination of the strong coupling constant from Transverse Energy-Energy Correlations in multijet events at 13 TeV with the ATLAS detector. The data sample with integrated luminosity of 139 inverse fb corresponds to proton-proton collisions collected by ATLAS during the LHC Run-2. Jets are reconstructed using the anti-kt algorithm with jet radius 0.4. The data sample is binned in HT2 defined as the sum of the transverse momentum of the two leading jets. The theoretical predictions are calculated at NNLO in perturbative QCD.

The selection criteria are defined as:
- HT2 &gt; 1 TeV
- ptJet &gt; 60 GeV
- |etaJet| &lt; 2.4
DOI: 10.17182/hepdata.135073.v1/t2
title: "Data TEEC 01" of "Determination of the strong coupling constant from transverse energy$-$energy correlations in multijet events at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Particle-level TEEC results for the first HT2 bin
description: CERN-LHC. Asymptotic freedom beyond the TeV scale and determination of the strong coupling constant from Transverse Energy-Energy Correlations in multijet events at 13 TeV with the ATLAS detector. The data sample with integrated luminosity of 139 inverse fb corresponds to proton-proton collisions collected by ATLAS during the LHC Run-2. Jets are reconstructed using the anti-kt algorithm with jet radius 0.4. The data sample is binned in HT2 defined as the sum of the transverse momentum of the two leading jets. The theoretical predictions are calculated at NNLO in perturbative QCD.

The selection criteria are defined as:
- HT2 &gt; 1 TeV
- ptJet &gt; 60 GeV
- |etaJet| &lt; 2.4
DOI: 10.17182/hepdata.135073.v1/t3
title: "Data TEEC 02" of "Determination of the strong coupling constant from transverse energy$-$energy correlations in multijet events at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Particle-level TEEC results for the second HT2 bin
description: CERN-LHC. Asymptotic freedom beyond the TeV scale and determination of the strong coupling constant from Transverse Energy-Energy Correlations in multijet events at 13 TeV with the ATLAS detector. The data sample with integrated luminosity of 139 inverse fb corresponds to proton-proton collisions collected by ATLAS during the LHC Run-2. Jets are reconstructed using the anti-kt algorithm with jet radius 0.4. The data sample is binned in HT2 defined as the sum of the transverse momentum of the two leading jets. The theoretical predictions are calculated at NNLO in perturbative QCD.

The selection criteria are defined as:
- HT2 &gt; 1 TeV
- ptJet &gt; 60 GeV
- |etaJet| &lt; 2.4
DOI: 10.17182/hepdata.135073.v1/t10
title: "Data TEEC 09" of "Determination of the strong coupling constant from transverse energy$-$energy correlations in multijet events at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Particle-level TEEC results for the ninth HT2 bin
description: CERN-LHC. Asymptotic freedom beyond the TeV scale and determination of the strong coupling constant from Transverse Energy-Energy Correlations in multijet events at 13 TeV with the ATLAS detector. The data sample with integrated luminosity of 139 inverse fb corresponds to proton-proton collisions collected by ATLAS during the LHC Run-2. Jets are reconstructed using the anti-kt algorithm with jet radius 0.4. The data sample is binned in HT2 defined as the sum of the transverse momentum of the two leading jets. The theoretical predictions are calculated at NNLO in perturbative QCD.

The selection criteria are defined as:
- HT2 &gt; 1 TeV
- ptJet &gt; 60 GeV
- |etaJet| &lt; 2.4