cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.110347.v1/t1
title: "Table 2d" of "Rapidity dependence of antiproton to proton ratios in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\overline{\mathrm{p}}/\mathrm{p}$ versus $\mathrm{Centrality}$ for $\overline{\mathrm{p}}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=130\,\mathrm{Ge\!V}$
description: Measurements, with the BRAHMS detector, of the antiproton to proton ratio at central and forward rapidities are presented for Au+Au reactions at sqrt{s_{NN}}=130 GeV, and for three different collision centralities. For collisions in the 0-40% centrality range we find $N(\bar{{\rm p}})/N({\rm p}) = 0.64 +- 0.04 (stat.) +- 0.06 (syst.) at y ~0, 0.66 +- 0.03 +- 0.06 at y ~ 0.7, and 0.41 +- 0.04 +- 0.06 at y ~ 2. The ratios are found to be nearly independent of collision centrality and transverse momentum. The measurements demonstrate that the antiproton and proton rapidity densities vary differently with rapidity, and indicate that a net-baryon free midrapidity plateau (Bjorken limit) is not reached at this RHIC energy.
DOI: 10.17182/hepdata.110347.v1/t2
title: "Table 2a" of "Rapidity dependence of antiproton to proton ratios in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\overline{\mathrm{p}}/\mathrm{p}$ versus $p_{\mathrm{T}}$ for $\overline{\mathrm{p}}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=130\,\mathrm{Ge\!V}$
description: Measurements, with the BRAHMS detector, of the antiproton to proton ratio at central and forward rapidities are presented for Au+Au reactions at sqrt{s_{NN}}=130 GeV, and for three different collision centralities. For collisions in the 0-40% centrality range we find $N(\bar{{\rm p}})/N({\rm p}) = 0.64 +- 0.04 (stat.) +- 0.06 (syst.) at y ~0, 0.66 +- 0.03 +- 0.06 at y ~ 0.7, and 0.41 +- 0.04 +- 0.06 at y ~ 2. The ratios are found to be nearly independent of collision centrality and transverse momentum. The measurements demonstrate that the antiproton and proton rapidity densities vary differently with rapidity, and indicate that a net-baryon free midrapidity plateau (Bjorken limit) is not reached at this RHIC energy.
DOI: 10.17182/hepdata.110347.v1/t3
title: "Table 2b" of "Rapidity dependence of antiproton to proton ratios in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\overline{\mathrm{p}}/\mathrm{p}$ versus $p_{\mathrm{T}}$ for $\overline{\mathrm{p}}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=130\,\mathrm{Ge\!V}$
description: Measurements, with the BRAHMS detector, of the antiproton to proton ratio at central and forward rapidities are presented for Au+Au reactions at sqrt{s_{NN}}=130 GeV, and for three different collision centralities. For collisions in the 0-40% centrality range we find $N(\bar{{\rm p}})/N({\rm p}) = 0.64 +- 0.04 (stat.) +- 0.06 (syst.) at y ~0, 0.66 +- 0.03 +- 0.06 at y ~ 0.7, and 0.41 +- 0.04 +- 0.06 at y ~ 2. The ratios are found to be nearly independent of collision centrality and transverse momentum. The measurements demonstrate that the antiproton and proton rapidity densities vary differently with rapidity, and indicate that a net-baryon free midrapidity plateau (Bjorken limit) is not reached at this RHIC energy.
DOI: 10.17182/hepdata.110347.v1/t4
title: "Table 2c" of "Rapidity dependence of antiproton to proton ratios in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\overline{\mathrm{p}}/\mathrm{p}$ versus $p_{\mathrm{T}}$ for $\overline{\mathrm{p}}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=130\,\mathrm{Ge\!V}$
description: Measurements, with the BRAHMS detector, of the antiproton to proton ratio at central and forward rapidities are presented for Au+Au reactions at sqrt{s_{NN}}=130 GeV, and for three different collision centralities. For collisions in the 0-40% centrality range we find $N(\bar{{\rm p}})/N({\rm p}) = 0.64 +- 0.04 (stat.) +- 0.06 (syst.) at y ~0, 0.66 +- 0.03 +- 0.06 at y ~ 0.7, and 0.41 +- 0.04 +- 0.06 at y ~ 2. The ratios are found to be nearly independent of collision centrality and transverse momentum. The measurements demonstrate that the antiproton and proton rapidity densities vary differently with rapidity, and indicate that a net-baryon free midrapidity plateau (Bjorken limit) is not reached at this RHIC energy.
DOI: 10.17182/hepdata.110347.v1/t5
title: "Table 3a" of "Rapidity dependence of antiproton to proton ratios in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\overline{\mathrm{p}}/\mathrm{p}$ versus $y$ for $\overline{\mathrm{p}}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=130\,\mathrm{Ge\!V}$
description: Measurements, with the BRAHMS detector, of the antiproton to proton ratio at central and forward rapidities are presented for Au+Au reactions at sqrt{s_{NN}}=130 GeV, and for three different collision centralities. For collisions in the 0-40% centrality range we find $N(\bar{{\rm p}})/N({\rm p}) = 0.64 +- 0.04 (stat.) +- 0.06 (syst.) at y ~0, 0.66 +- 0.03 +- 0.06 at y ~ 0.7, and 0.41 +- 0.04 +- 0.06 at y ~ 2. The ratios are found to be nearly independent of collision centrality and transverse momentum. The measurements demonstrate that the antiproton and proton rapidity densities vary differently with rapidity, and indicate that a net-baryon free midrapidity plateau (Bjorken limit) is not reached at this RHIC energy.
DOI: 10.17182/hepdata.110347.v1/t6
title: "Table 3b" of "Rapidity dependence of antiproton to proton ratios in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\mathrm{\pi}^{-}/\mathrm{\pi}^{+}$ versus $y$ for $\mathrm{\pi}^{-}$, $\mathrm{\pi}^{+}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=130\,\mathrm{Ge\!V}$
description: Measurements, with the BRAHMS detector, of the antiproton to proton ratio at central and forward rapidities are presented for Au+Au reactions at sqrt{s_{NN}}=130 GeV, and for three different collision centralities. For collisions in the 0-40% centrality range we find $N(\bar{{\rm p}})/N({\rm p}) = 0.64 +- 0.04 (stat.) +- 0.06 (syst.) at y ~0, 0.66 +- 0.03 +- 0.06 at y ~ 0.7, and 0.41 +- 0.04 +- 0.06 at y ~ 2. The ratios are found to be nearly independent of collision centrality and transverse momentum. The measurements demonstrate that the antiproton and proton rapidity densities vary differently with rapidity, and indicate that a net-baryon free midrapidity plateau (Bjorken limit) is not reached at this RHIC energy.
DOI: 10.17182/hepdata.110427.v1/t1
title: "Figure 2" of "Measurement of Direct Photons in Au+Au Collisions at sqrt(s_NN) = 200 GeV"

description: Direct photon spectra for all centrality selections in Au+Au.
description: BNL-RHIC. We report the measurement of direct photons at midrapidity in Au+Au collisions at $\sqrt{s_{NN}}$=200GeV. The direct photon signal was extracted for the transverse momentum range of 4 GeV/c &lt;$p_T$&lt;22 GeV/c, using a statistical method to subtract decay photons from the inclusive photon sample.The direct-photon nuclear-modification factor $R_{AA}$ was calculated as a function of $p_T$ for different Au+Au collision centralities using the measured p+p direct-photon spectrum and compared totheoretical predictions.$R_{AA}$ was found to be consistent with unity for all centralities over theentire measuredpTrange. Theoretical models that account for modifications ofinitial-direct-photonproduction due to modified-parton-distribution functions(PDFs) in Au and the different isospin composition of the nuclei predict a modest change of $R_{AA}$ from unity. They are consistent with the data. Models with compensating effects of the quark-gluon plasma on high-energy photons,such as suppression of jet-fragmentation photons and induced-photon bremsstrahlung from partonstraversing the medium, are also consistent with this measurement.
DOI: 10.25549/vercoutere-ouc110609973
title: Parade of military men

description: Parade (?) of military males, some carrying swords or rifles; bystanders in the lower right corner watching. Greenish faces, dressed in purple, orange, blue, and green uniforms. Pink and orange background. Notes on reverse side by OT: Did this with a great deal of pleasure expressed on his face. Asked me if he couldn't do something in oils--says he has never worked with oils and would like to try
DOI: 10.17182/hepdata.110427.v1/t2
title: "Figure 3-4" of "Measurement of Direct Photons in Au+Au Collisions at sqrt(s_NN) = 200 GeV"

description: Direct photon nuclear modification factor ($R_{AA}$)
description: BNL-RHIC. We report the measurement of direct photons at midrapidity in Au+Au collisions at $\sqrt{s_{NN}}$=200GeV. The direct photon signal was extracted for the transverse momentum range of 4 GeV/c &lt;$p_T$&lt;22 GeV/c, using a statistical method to subtract decay photons from the inclusive photon sample.The direct-photon nuclear-modification factor $R_{AA}$ was calculated as a function of $p_T$ for different Au+Au collision centralities using the measured p+p direct-photon spectrum and compared totheoretical predictions.$R_{AA}$ was found to be consistent with unity for all centralities over theentire measuredpTrange. Theoretical models that account for modifications ofinitial-direct-photonproduction due to modified-parton-distribution functions(PDFs) in Au and the different isospin composition of the nuclei predict a modest change of $R_{AA}$ from unity. They are consistent with the data. Models with compensating effects of the quark-gluon plasma on high-energy photons,such as suppression of jet-fragmentation photons and induced-photon bremsstrahlung from partonstraversing the medium, are also consistent with this measurement.
DOI: 10.17182/hepdata.110430.v1/t1
title: "Table 3" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: The total $b \bar{b}$-dijet and $c \bar{c}$-dijet cross-sections and their ratio in the fiducial region, compared with the NLO predictions. The first uncertainty is the combined statistical and systematic uncertainty and the second is the uncertainty from the luminosity. For the predictions, the first uncertainty corresponds to the scale uncertainty, the second to the PDF uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t2
title: "Table 4" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Numerical results of $b \bar{b}$- and $c \bar{c}$-dijet cross-sections, $c \bar{c}$/$b \bar{b}$ dijet cross-section ratios and their total uncertainties as a function of the leading jet $\eta$ (pseudorapidity).
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t3
title: "Table 5" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Numerical results of $b \bar{b}$- and $c \bar{c}$-dijet cross-sections, $c \bar{c}$/$b \bar{b}$ dijet cross-section ratios and their total uncertainties as a function of $\Delta y^*$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t4
title: "Table 6" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Numerical results of $b \bar{b}$- and $c \bar{c}$-dijet cross-sections, $c \bar{c}$/$b \bar{b}$ dijet cross-section ratios and their total uncertainties as a function of the leading jet $p_T$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t5
title: "Table 7" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Numerical results of $b \bar{b}$- and $c \bar{c}$-dijet cross-sections, $c\bar{c}$/$b \bar{b}$ dijet cross-section ratios and their total uncertainties as a function of $m_{jj}$ (dijet invariant mass).
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t6
title: "Table 8" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet eta intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t7
title: "Table 9" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet eta intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t8
title: "Table 10" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $\eta$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is nb$^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t10
title: "Table 12" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the $\Delta y^*$ intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t11
title: "Table 13" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the $\Delta y^*$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is nb$^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t12
title: "Table 14" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $p_T$ intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c)^2$ and the $p_T$ intervals are given in GeV$/c$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t13
title: "Table 15" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $p_T$ intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c)^2$ and the $p_T$ intervals are given in GeV$/$c .
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t9
title: "Table 11" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the $\Delta y^*$ intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc110609968
title: Jungle scene with plants and vines

description: Green, black, and blue jungle scene with plants and vines
DOI: 10.17182/hepdata.110430.v1/t14
title: "Table 16" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $p_T$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c)^2$ and the $p_T$ intervals are given in GeV$/c$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t15
title: "Table 17" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the $m_{jj}$ intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c^2)^2$ and the mass intervals are given in GeV$/c^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t16
title: "Table 18" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the $m_{jj}$ intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c^2)^2$ and the mass intervals are given in GeV$/c^2$.
description: No data abstract available.
DOI: 10.17182/hepdata.110430.v1/t17
title: "Table 19" of "Measurement of differential $b\bar{b}$- and $c\bar{c}$-dijet cross-sections in the forward region of $pp$ collisions at $\sqrt{s}=13 ~ \mathrm{TeV}$"

description: Covariance matrix, corresponding to the total uncertainties, obtained between the $m_{jj}$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is $($nb GeV$/c^2)^2$ and the mass intervals are given in GeV$/c^2$.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc110610046
title: A good dog is a woman's best friend

description: Three nude females: one with yellow body, red head, and brown hair, wearing a yellow crown sitting on brown rocks with one leg up next to a tree, with a brown dog on her lap and licking her; one with a red body and head with black hair standing and reaching out to red birds; one with a red body and head with brown hair standing next to a tree with a brown dog standing against her and licking her; a few words written on top of the painting including "A good dog is a woman best friend;" two standing females are enclosed in a frame with a green background; the background in the other section is brown, red, and orange. Note on the reverse side by OT: #3. See description of 347 for OT notes.
DOI: 10.25549/vercoutere-ouc110610063
title: Word salad about sales tax passage

description: Straight lines drawn in pencil and covered with a word salad printed in blue ink; words understandable but nonsensical; includes the following words "A measure designed to levy 10 cents sales tax was given final passag [sic] today," "like to paint or draw sexuals." See description of 347 for OT notes.
DOI: 10.17182/hepdata.110657.v1/t1
title: "Data from Figure 2(a)1" of "Probing Strangeness Canonical Ensemble with $K^{-}$, $\phi(1020)$ and $\Xi^{-}$ Production in Au+Au Collisions at ${\sqrt{s_{NN}} = {3\,GeV}}$"

description: $K^-$ (a), invariant yields as a function of $m_T-m_0$ for various rapidity regions in 0--10\% central Au+Au collisions at ${\sqrt{s_{\mathrm{NN}}} = \mathrm{3\,GeV}}$. Statistics and systematic uncertainties are added quadratic here for plotting. Solid and dashed black lines depict $m_T$ exponential function fits to the measured data points with arbitrate scaling factors in each rapidity windows.
description: BNL-RHIC. We report on the first multi-differential measurement of $\phi$ meson and $\Xi^{-}$ hyperon production as well as the $\phi/K^-$ and $\phi/\Xi^-$ ratio in Au+Au collisions at ${\sqrt{s_{\mathrm{NN}}} = \mathrm{3\,GeV}}$ with the STAR experiment under its fixed target configuration at RHIC. $\phi$ mesons and $\Xi^{-}$ hyperons are measured through their hadronic decay channels, $\phi\rightarrow K^+K^-$ and $\Xi^-\rightarrow \Lambda\pi^-$. The transverse kinetic energy spectra of $K^-$, $\phi$ and $\Xi^{-}$ are presented in different centrality and rapidity intervals. The total production yields and the ratios within a $4\pi$ coverage are calculated and compared to thermal model predictions. The calculation within grand canonical ensemble framework shows a clear discrepancy from our measurement. Our data favors the canonical ensemble approach employing local strangeness conservation with a small strangeness correlation length ($r_c \leq 4.2$\,fm) in $\mathrm{0--10\%}$ central Au+Au collisions at ${\sqrt{s_{\mathrm{NN}}} = \mathrm{3\,GeV}}$.
DOI: 10.17182/hepdata.110657.v1/t2
title: "Data from Figure 2(a)2" of "Probing Strangeness Canonical Ensemble with $K^{-}$, $\phi(1020)$ and $\Xi^{-}$ Production in Au+Au Collisions at ${\sqrt{s_{NN}} = {3\,GeV}}$"

description: $\phi$ meson (b) invariant yields as a function of $m_T-m_0$ for various rapidity regions in 0--10\% central Au+Au collisions at ${\sqrt{s_{\mathrm{NN}}} = \mathrm{3\,GeV}}$. Statistics and systematic uncertainties are added quadratic here for plotting. Solid and dashed black lines depict $m_T$ exponential function fits to the measured data points with arbitrate scaling factors in each rapidity windows.
description: BNL-RHIC. We report on the first multi-differential measurement of $\phi$ meson and $\Xi^{-}$ hyperon production as well as the $\phi/K^-$ and $\phi/\Xi^-$ ratio in Au+Au collisions at ${\sqrt{s_{\mathrm{NN}}} = \mathrm{3\,GeV}}$ with the STAR experiment under its fixed target configuration at RHIC. $\phi$ mesons and $\Xi^{-}$ hyperons are measured through their hadronic decay channels, $\phi\rightarrow K^+K^-$ and $\Xi^-\rightarrow \Lambda\pi^-$. The transverse kinetic energy spectra of $K^-$, $\phi$ and $\Xi^{-}$ are presented in different centrality and rapidity intervals. The total production yields and the ratios within a $4\pi$ coverage are calculated and compared to thermal model predictions. The calculation within grand canonical ensemble framework shows a clear discrepancy from our measurement. Our data favors the canonical ensemble approach employing local strangeness conservation with a small strangeness correlation length ($r_c \leq 4.2$\,fm) in $\mathrm{0--10\%}$ central Au+Au collisions at ${\sqrt{s_{\mathrm{NN}}} = \mathrm{3\,GeV}}$.