{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.139721.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2093738"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2023","description":"This Letter reports on the first measurements of transverse momentum dependent flow angle $\\Psi_{n}$ and flow magnitude $v_{n}$ fluctuations, determined using new four-particle correlators. The measurements are performed for various centralities in Pb-\u2013Pb collisions at a centre of mass energy of $\\sqrt{s_{\\rm NN}} = 5.02{\\rm\\ TeV}$ with ALICE at the LHC. Both flow angle and flow magnitude fluctuations are observed in the presented centrality ranges and are strongest in the most central collisions and for a transverse momentum $p_{\\rm T} &gt; 2{\\rm\\ GeV}/c$. Comparison with theoretical models, including iEBE-VISHNU, MUSIC, and AMPT, show that the measurements bring novel insights into the fluctuating initial conditions that are not well known. In addition, these new results exhibit unique sensitivities to the specific shear viscosity, $\\eta/s$, of the quark\u2013gluon plasma (QGP) and to the initial state of the heavy-ion collisions. As such fluctuations are getting stronger with increasing $p_{\\rm T}$, a re-examination of existing models is needed to have a more precise and unbiased extraction of properties of the QGP.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.139721.v1/t1","@type":"Dataset","description":"The flow angle fluctuation $A_{\\rm 2}^{\\rm f}$ as a function of $p_{\\rm T}^{\\rm a}$ in different centrality classes","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.139721.v1/t2","@type":"Dataset","description":"The flow magnitude fluctuation $M_{\\rm 2}^{\\rm f}$ as a function of $p_{\\rm T}^{\\rm a}$ in different centrality classes","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.139721.v1/t3","@type":"Dataset","description":"Lower (upper) limit of flow angle (magnitude) fluctuations and flow vector fluctuations as a function of centrality for 3.0 &lt;...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.139721.v1/t4","@type":"Dataset","description":"Ratio of lower (upper) flow angle (magnitude) fluctuation limits to total flow vector fluctuations as a function of centrality for...","name":"Table 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2093738?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/139721"}],"inLanguage":"en","name":"Observation of flow angle and flow magnitude fluctuations in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV at the LHC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2093738?version=1","version":1}
