Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3755
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dc.contributor.authorBHALERAO, RAJEEV S.en_US
dc.contributor.authorGiacalone, Giulianoen_US
dc.contributor.authorGuerrero-Rodríguezc , Pabloen_US
dc.contributor.authorLuzumd, Matthewen_US
dc.contributor.authorMarquete , Cyrilleen_US
dc.contributor.authorOllitraultb, Jean-Yvesen_US
dc.date.accessioned2019-07-24T05:29:58Z
dc.date.available2019-07-24T05:29:58Z
dc.date.issued2019-06en_US
dc.identifier.citationActa Physica Polonica B, 50(6), 1165-1176.en_US
dc.identifier.issn0587-4254en_US
dc.identifier.issn1509-5770en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3755-
dc.identifier.urihttps://doi.org/10.5506/APhysPolB.50.1165en_US
dc.description.abstractThe magnitude of anisotropic flow in a nucleus-nucleus collision is determined by the energy-density field, rho(x; y; z), created right after the collision occurs. Specifically, elliptic flow, v(2), and triangular flow, v(3), are proportional to the anisotropy coefficients epsilon(2) and epsilon(3), which are functionals of rho. We express the mean and the variance of epsilon(2) and epsilon(3) as a function of the 1- and 2-point functions of rho. These results generalize results obtained previously that were valid only for central collisions or only for identical point-like sources. We apply them to the color glass condensate effective theory using the recently derived expression of the 2-point function.en_US
dc.language.isoenen_US
dc.publisherJagiellonian University Pressen_US
dc.subjectPhysicsen_US
dc.subjectTOC-JUL-2019en_US
dc.subject2019en_US
dc.titleRelating Eccentricity Fluctuations to Density Fluctuations in Heavy-ion Collisionsen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleActa Physica Polonica Ben_US
dc.publication.originofpublisherForeignen_US
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