| Home > Publications database > Polarization of $\Lambda$ and $\overline{\Lambda}$ hyperons along the beam direction in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV > print |
| 001 | 251005 | ||
| 005 | 20250630143456.0 | ||
| 024 | 7 | _ | |a 10.17182/HEPDATA.128775 |2 doi |
| 037 | _ | _ | |a GSI-2023-00206 |
| 041 | _ | _ | |a English |
| 100 | 1 | _ | |a ALICE Collaboration |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
| 245 | _ | _ | |a Polarization of $\Lambda$ and $\overline{\Lambda}$ hyperons along the beam direction in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV |
| 260 | _ | _ | |c 2022 |
| 336 | 7 | _ | |a MISC |2 BibTeX |
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| 336 | 7 | _ | |a Chart or Table |0 26 |2 EndNote |
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| 336 | 7 | _ | |a DATA_SET |2 ORCID |
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| 500 | _ | _ | |a Journal Article GSI record: GSI-2023-00143 |
| 520 | _ | _ | |a The polarization of the $\Lambda$ and $\overline\Lambda$ hyperons along the beam ($z$) direction, $P_{\rm z}$, has been measured in Pb--Pb collisions at $\sqrt{s_{\rm NN}} =$ 5.02 TeV recorded with ALICE at the Large Hadron Collider (LHC). The largest contribution to $P_{\rm z}$ comes from elliptic flow induced vorticity and can be characterized by the second Fourier sine coefficient $P_{\rm z,\,{\rm s2}} = \langle{P_{\rm z}\sin(2\varphi - 2 \Psi_{\rm 2})}\rangle$, where $\varphi$ is the hyperon azimuthal emission angle, and $\Psi_{\rm 2}$ is the elliptic flow plane angle. We report the measurement of $P_{\rm z,\,{\rm s2}}$ for different collision centralities, and in the 30--50\% centrality interval as a function of the hyperon transverse momentum ($p_{\rm T}$) and rapidity ($y_{\rm H}$). |
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| 773 | _ | _ | |a 10.17182/HEPDATA.128775 |
| 787 | 0 | _ | |a Acharya, Shreyasi et.al. |d College Park, Md. : APS, 2022 |i RelatedTo |0 GSI-2023-00143 |r arXiv:2107.11183 ; CERN-EP-2021-148 |t Polarization of $\Lambda$ and $\bar \Lambda$ Hyperons along the Beam Direction in Pb-Pb Collisions at $\sqrt {s_{NN}}$ = 5.02 TeV |
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