Paper proposal: Hyper-Nuclei He4L Production in √s_NN = 3 GeV Au+Au collisions at RHIC
Updated on Fri, 2024-06-28 09:28. Originally created by fzhao on 2024-06-17 04:21.
PAs: L.B. Chen, X.H. He, C.L. Hu, Y.J. Ji, X.J. Li, Y.H. Leung, X.F. Luo, G.N. Xie, N. Xu, Y.P. Zhang, F.Y. Zhao, Y.F. Zhang
https://www.overleaf.com/read/bhgmntznpwzf#04c55c
Analysis note:
https://www.overleaf.com/read/xzjbtqyprcxh#c8bba3
Supplemental materials:
PWG Presentations:
https://drupal.star.bnl.gov/STAR/event/2024/03/11/LFSUPC-PWG-meeting/He4L-production-3-GeV-AuAu-Collisions
https://drupal.star.bnl.gov/STAR/system/files/He4L_production_3GeVAuAu_FengyiZhao_20230619.pdf
https://drupal.star.bnl.gov/STAR/system/files/Update_for_He4_%20Production_Analysis_20240520_0.pdf
Collaboration Meeting:
https://drupal.star.bnl.gov/STAR/meetings/STAR-Collaboration-Meeting-March-2024/LFSUPC-Parallel-Session-II/He4L-AuAu-collisions-30-Ge
Paper Proposal on PWG
https://drupal.star.bnl.gov/STAR/system/files/fzhao_He4LProduction_20240422_PaperProposal.pdf
PWGC Review:
https://drupal.star.bnl.gov/STAR/system/files/fzhao_He4LProduction_PWGC.pdf
Target journal: Chinese Physics C
Bookmarks: Abstract Figures Paper draft Note Supplemental materials
Abstract:
Hypernuclei, bound states of nuclei with one or more hyperons, serve as a natural laboratory to investigate the hyperon-nucleon interaction. Hypernuclei production in heavy-ion collisions at high-baryon density region, shall provide valuable information for studying hyper-cluster formation mechanism. In Au+Au collisions at √s_NN = 3 GeV preformed by the STAR experiment, hyper-nuclei He4L are identified by its three-body decay channel, i.e He4L->3He +p+π-, and He4L yield as a function of rapidity and transverse momentum in 0-50% centrality are measured for first time. We found that yields of He4L along the rapidity are overall lower than these of H4L, and differential yield ratios of He4L/H4L are consistent with these of He3/t within uncertainties. The observed yield ratios can be described by both the JAM plus an afterburner coalescence and canonical thermal model.
Proposed figures:
![](/STAR/system/files/userfiles/6593/image/Figure_PID3GeV_He4L_version2.png)
Figure 1: Rigidity (p/q) verses energy loss ⟨dE/dx⟩ obtained with the TPC detector in √s_NN = 3.0 GeV Au+Au collisions, lines represents the Bichsel functions for different particle species.
![](/STAR/system/files/userfiles/6593/image/invariantMass_acceptance_miniCut_expData_logScale_v5.png)
Figure 2: (Left panel) Invariant mass of He3+p+pi distributions from √s_NN = 3.0 GeV Au+Au collisions. Open circle and filled-red-circles are raw data and background subtracted distributions, respectively; (right panel) Acceptance of the He4L raw yields shown in transverse momentum pT vs. rapidity y.
![](/STAR/system/files/userfiles/6593/image/d2Ndydpt_BlastWave_Boltzmann_4raps_rawFit_over_eff_model_noH4L_v4.png)
Figure 3: Transverse momentum distributions d2N/pTdydpT of He4L from 0-50\% central √s_NN=3.0 GeV Au+Au collisions. Data points from four rapidity bins are shown. Blast-wave fit results are shown as dashed-lines while the JAM plus afterburner coalescence model results are shown as blue bands.
![](/STAR/system/files/userfiles/6593/image/dNdy_meanPt_combine_model_v7.png)
Figure 4: (Left panel) Rapidity dependence of the He4L yields (filled-black-circle) from 0-50% central √s_NN = 3.0 GeV Au+Au collisions; (right panel) Rapidity dependence of the averaged transverse momentum <pT> of He4L. For comparison, the results of H4L are also shown as Green triangles. Model calculations from JAM plus afterburner coalescence are shown as orange- and green-lines for He4L and H4L, respectively.
![](/STAR/system/files/userfiles/6593/image/ratios_He3_vs_t_He4L_vs_H4L_Liubing_model_thermal_v5.png)
Figure 5: Rapidity dependence of the yield ratio for He4L/H4L (filled circle) and He3/t (open triangle) from the 0-50% √s_NN = 3.0 GeV Au+Au collisions. He4L/H4L yield ratio given by the JAM model plus afterburner coalescence is shown as the blue band. Yield ratios of He4L/H4L and He3/t given by the thermal model are shown by magenta and gray lines, respectively.
Conclusions:
Bookmarks: Abstract Figures Paper draft Note Supplemental materials
Abstract:
Hypernuclei, bound states of nuclei with one or more hyperons, serve as a natural laboratory to investigate the hyperon-nucleon interaction. Hypernuclei production in heavy-ion collisions at high-baryon density region, shall provide valuable information for studying hyper-cluster formation mechanism. In Au+Au collisions at √s_NN = 3 GeV preformed by the STAR experiment, hyper-nuclei He4L are identified by its three-body decay channel, i.e He4L->3He +p+π-, and He4L yield as a function of rapidity and transverse momentum in 0-50% centrality are measured for first time. We found that yields of He4L along the rapidity are overall lower than these of H4L, and differential yield ratios of He4L/H4L are consistent with these of He3/t within uncertainties. The observed yield ratios can be described by both the JAM plus an afterburner coalescence and canonical thermal model.
Proposed figures:
![](/STAR/system/files/userfiles/6593/image/Figure_PID3GeV_He4L_version2.png)
Figure 1: Rigidity (p/q) verses energy loss ⟨dE/dx⟩ obtained with the TPC detector in √s_NN = 3.0 GeV Au+Au collisions, lines represents the Bichsel functions for different particle species.
![](/STAR/system/files/userfiles/6593/image/invariantMass_acceptance_miniCut_expData_logScale_v5.png)
Figure 2: (Left panel) Invariant mass of He3+p+pi distributions from √s_NN = 3.0 GeV Au+Au collisions. Open circle and filled-red-circles are raw data and background subtracted distributions, respectively; (right panel) Acceptance of the He4L raw yields shown in transverse momentum pT vs. rapidity y.
![](/STAR/system/files/userfiles/6593/image/d2Ndydpt_BlastWave_Boltzmann_4raps_rawFit_over_eff_model_noH4L_v4.png)
Figure 3: Transverse momentum distributions d2N/pTdydpT of He4L from 0-50\% central √s_NN=3.0 GeV Au+Au collisions. Data points from four rapidity bins are shown. Blast-wave fit results are shown as dashed-lines while the JAM plus afterburner coalescence model results are shown as blue bands.
![](/STAR/system/files/userfiles/6593/image/dNdy_meanPt_combine_model_v7.png)
Figure 4: (Left panel) Rapidity dependence of the He4L yields (filled-black-circle) from 0-50% central √s_NN = 3.0 GeV Au+Au collisions; (right panel) Rapidity dependence of the averaged transverse momentum <pT> of He4L. For comparison, the results of H4L are also shown as Green triangles. Model calculations from JAM plus afterburner coalescence are shown as orange- and green-lines for He4L and H4L, respectively.
![](/STAR/system/files/userfiles/6593/image/ratios_He3_vs_t_He4L_vs_H4L_Liubing_model_thermal_v5.png)
Figure 5: Rapidity dependence of the yield ratio for He4L/H4L (filled circle) and He3/t (open triangle) from the 0-50% √s_NN = 3.0 GeV Au+Au collisions. He4L/H4L yield ratio given by the JAM model plus afterburner coalescence is shown as the blue band. Yield ratios of He4L/H4L and He3/t given by the thermal model are shown by magenta and gray lines, respectively.
Conclusions:
- Production of He4L are measured via both 3-body decay channel in √s_NN = 3 GeV Au+Au collisions at RHIC.
- Yields of He4L along the rapidity are overall consistent with these of H4L within 1 sigma uncertainties, except for the middle rapidity region -0.2<y<0, which is 2.4 sigma lower than the yield of H4L. Yield ratios of He4L/H4L are consistent with that of He3/t within uncertainties.
- With the same coalescence parameters for He3-Λ and t-Λ, calculations from the transport model JAM plus coalescence afterburner can reproduce both the yield and mean pT distributions for He4L and H4L, as well as the He4L/H4L and 3He/t yields ratios. Thermal-fist predictions with Tcℎ=75MeV and μB=750MeV can reasonably describe both ratios.
- These results imply that the production mechanism for He4L from He3-Λ and H4L from t-Λ are the same within uncertainties.
https://www.overleaf.com/read/bhgmntznpwzf#04c55c
Analysis note:
https://www.overleaf.com/read/xzjbtqyprcxh#c8bba3
Supplemental materials:
PWG Presentations:
https://drupal.star.bnl.gov/STAR/event/2024/03/11/LFSUPC-PWG-meeting/He4L-production-3-GeV-AuAu-Collisions
https://drupal.star.bnl.gov/STAR/system/files/He4L_production_3GeVAuAu_FengyiZhao_20230619.pdf
https://drupal.star.bnl.gov/STAR/system/files/Update_for_He4_%20Production_Analysis_20240520_0.pdf
Collaboration Meeting:
https://drupal.star.bnl.gov/STAR/meetings/STAR-Collaboration-Meeting-March-2024/LFSUPC-Parallel-Session-II/He4L-AuAu-collisions-30-Ge
Paper Proposal on PWG
https://drupal.star.bnl.gov/STAR/system/files/fzhao_He4LProduction_20240422_PaperProposal.pdf
PWGC Review:
https://drupal.star.bnl.gov/STAR/system/files/fzhao_He4LProduction_PWGC.pdf
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