002007002 001__ 2007002 002007002 003__ SzGeCERN 002007002 005__ 20220810150836.0 002007002 0248_ $$aoai:cds.cern.ch:2007002$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT 002007002 0247_ $$2DOI$$a10.1103/PhysRevC.92.034903 002007002 035__ $$9arXiv$$aoai:arXiv.org:1504.01289 002007002 035__ $$9Inspire$$a1357991 002007002 037__ $$9arXiv$$aarXiv:1504.01289$$chep-ex 002007002 037__ $$aCERN-PH-EP-2015-079 002007002 041__ $$aeng 002007002 088__ $$aCERN-PH-EP-2015-079 002007002 084__ $$2CERN Library$$aPH-EP-2015-079 002007002 100__ $$aAad, Georges$$iINSPIRE-00210391$$uMarseille, CPPM$$vCPPM , Aix-Marseille Université and CNRS/IN2P3, Marseille, France 002007002 245__ $$aMeasurement of the correlation between flow harmonics of different order in lead-lead collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS detector 002007002 246__ $$9arXiv$$aMeasurement of the correlation between flow harmonics of different order in lead-lead collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS detector 002007002 269__ $$aGeneva$$bCERN$$c06 Apr 2015 002007002 260__ $$c2015-09-14 002007002 300__ $$a30 p 002007002 500__ $$9arXiv$$a22 pages plus author list + cover pages (35 pages total), 16 figures, submitted to Phys. Rev. C., All figures including auxiliary figures can be found at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2014-03/ 002007002 520__ $$aCorrelations between the elliptic or triangular flow coefficients $v_m$ ($m$=2 or 3) and other flow harmonics $v_n$ ($n$=2 to 5) are measured using $\sqrt{s_{NN}}=2.76$ TeV Pb+Pb collision data collected in 2010 by the ATLAS experiment at the LHC, corresponding to an integrated lumonisity of 7 $\mu$b$^{-1}$. The $v_m$-$v_n$ correlations are measured in midrapidity as a function of centrality, and, for events within the same centrality interval, as a function of event ellipticity or triangularity defined in a forward rapidity region. For events within the same centrality interval, $v_3$ is found to be anticorrelated with $v_2$ and this anticorrelation is consistent with similar anticorrelations between the corresponding eccentricities $\epsilon_2$ and $\epsilon_3$. On the other hand, it is observed that $v_4$ increases strongly with $v_2$, and $v_5$ increases strongly with both $v_2$ and $v_3$. The trend and strength of the $v_m$-$v_n$ correlations for $n$=4 and 5 are found to disagree with $\epsilon_m$-$\epsilon_n$ correlations predicted by initial-geometry models. Instead, these correlations are found to be consistent with the combined effects of a linear contribution to $v_n$ and a nonlinear term that is a function of $v_2^2$ or of $v_2v_3$, as predicted by hydrodynamic models. A simple two-component fit is used to separate these two contributions. The extracted linear and nonlinear contributions to $v_4$ and $v_5$ are found to be consistent with previously measured event-plane correlations. 002007002 520__ $$9HEPDATA$$hCERN-LHC. Experimental measurements of the correlations between the elliptic or triangular flow coefficients, $v_m$ ($m=2$ or 3), and other flow harmonics, $v_n$ ($n=2$ to 5) in lead-lead collisions. The data tables are linked to the corresponding figure number in the paper as well as additional plots in reference. 002007002 520__ $$9APS$$aCorrelations between the elliptic or triangular flow coefficients vm (m=2 or 3) and other flow harmonics vn (n=2 to 5) are measured using sNN=2.76 TeV Pb+Pb collision data collected in 2010 by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 7 μb−1. The vm-vn correlations are measured in midrapidity as a function of centrality, and, for events within the same centrality interval, as a function of event ellipticity or triangularity defined in a forward rapidity region. For events within the same centrality interval, v3 is found to be anticorrelated with v2 and this anticorrelation is consistent with similar anticorrelations between the corresponding eccentricities, ε2 and ε3. However, it is observed that v4 increases strongly with v2, and v5 increases strongly with both v2 and v3. The trend and strength of the vm-vn correlations for n=4 and 5 are found to disagree with εm-εn correlations predicted by initial-geometry models. Instead, these correlations are found to be consistent with the combined effects of a linear contribution to vn and a nonlinear term that is a function of v22 or of v2v3, as predicted by hydrodynamic models. A simple two-component fit is used to separate these two contributions. The extracted linear and nonlinear contributions to v4 and v5 are found to be consistent with previously measured event-plane correlations. 002007002 520__ $$9arXiv$$aCorrelations between the elliptic or triangular flow coefficients $v_m$ ($m$=2 or 3) and other flow harmonics $v_n$ ($n$=2 to 5) are measured using $\sqrt{s_{NN}}=2.76$ TeV Pb+Pb collision data collected in 2010 by the ATLAS experiment at the LHC, corresponding to an integrated lumonisity of 7 $\mu$b$^{-1}$. The $v_m$-$v_n$ correlations are measured in midrapidity as a function of centrality, and, for events within the same centrality interval, as a function of event ellipticity or triangularity defined in a forward rapidity region. For events within the same centrality interval, $v_3$ is found to be anticorrelated with $v_2$ and this anticorrelation is consistent with similar anticorrelations between the corresponding eccentricities $\epsilon_2$ and $\epsilon_3$. On the other hand, it is observed that $v_4$ increases strongly with $v_2$, and $v_5$ increases strongly with both $v_2$ and $v_3$. The trend and strength of the $v_m$-$v_n$ correlations for $n$=4 and 5 are found to disagree with $\epsilon_m$-$\epsilon_n$ correlations predicted by initial-geometry models. Instead, these correlations are found to be consistent with the combined effects of a linear contribution to $v_n$ and a nonlinear term that is a function of $v_2^2$ or of $v_2v_3$, as predicted by hydrodynamic models. A simple two-component fit is used to separate these two contributions. The extracted linear and nonlinear contributions to $v_4$ and $v_5$ are found to be consistent with previously measured event-plane correlations. 002007002 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/ 002007002 540__ $$3preprint$$aCC-BY-4.0 002007002 540__ $$3publication$$aCC-BY-3.0 002007002 542__ $$3preprint$$dCERN$$g2015 002007002 542__ $$3publication$$dCERN$$g2015 002007002 595__ $$aLANL EDS 002007002 595__ $$aCERN-PH-EP 002007002 65017 $$2arXiv$$aParticle Physics - Experiment 002007002 65027 $$2arXiv$$aNuclear Physics - Experiment 002007002 693__ $$aCERN LHC$$eATLAS 002007002 695__ $$9LANL EDS$$ahep-ex 002007002 695__ $$9LANL EDS$$anucl-ex 002007002 690C_ $$aARTICLE 002007002 690C_ $$aCERN 002007002 690C_ $$aATLAS_Papers 002007002 700__ $$aAbbott, Brad$$iINSPIRE-00060668$$uOklahoma U. 002007002 700__ $$aAbdallah, Jalal$$iINSPIRE-00305555$$uTaiwan, Inst. 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London 002007002 700__ $$aCampoverde, Angel$$iINSPIRE-00349667$$uSUNY, Stony Brook 002007002 700__ $$aCanale, Vincenzo$$iINSPIRE-00211960$$uINFN, Naples$$uNaples U. 002007002 700__ $$aCanepa, Anadi$$iINSPIRE-00045497$$uTRIUMF 002007002 700__ $$aCano Bret, Marc$$iINSPIRE-00361241$$uQueen Mary, U. of London 002007002 700__ $$aCantero, Josu$$iINSPIRE-00211972$$uMadrid, Autonoma U. 002007002 700__ $$aCantrill, Robert$$iINSPIRE-00235969$$uLIP, Lisbon 002007002 700__ $$aCao, Tingting$$iINSPIRE-00334314$$uSouthern Methodist U. 002007002 700__ $$aCapeans Garrido, Maria Del Mar$$iINSPIRE-00083814$$uCERN 002007002 700__ $$aCaprini, Irinel$$iINSPIRE-00070986$$uBucharest, IFIN-HH 002007002 700__ $$aCaprini, Mihai$$iINSPIRE-00211990$$uBucharest, IFIN-HH 002007002 700__ $$aCapua, Marcella$$iINSPIRE-00053925$$uINFN, Cosenza$$uCalabria U. 002007002 700__ $$aCaputo, Regina$$iINSPIRE-00212010$$uMainz U. 002007002 700__ $$aCardarelli, Roberto$$iINSPIRE-00212037$$uINFN, Rome 002007002 700__ $$aCarli, Tancredi$$iINSPIRE-00212045$$uCERN 002007002 700__ $$aCarlino, Gianpaolo$$iINSPIRE-00212057$$uINFN, Naples 002007002 700__ $$aCarminati, Leonardo$$iINSPIRE-00212069$$uINFN, Milan$$uMilan U. 002007002 700__ $$aCaron, Sascha$$iINSPIRE-00057327$$uNIKHEF, Amsterdam 002007002 700__ $$aCarquin, Edson$$iINSPIRE-00023484$$uChile U., Catolica 002007002 700__ $$aCarrillo-Montoya, German D$$iINSPIRE-00212072$$uTexas U., Arlington 002007002 700__ $$aCarter, Janet$$iINSPIRE-00149979$$uCambridge U. 002007002 700__ $$aCarvalho, João$$iINSPIRE-00226606$$uLIP, Lisbon$$uCoimbra U. 002007002 700__ $$aCasadei, Diego$$iINSPIRE-00212084$$uUniversity Coll. London 002007002 700__ $$aCasado, Maria Pilar$$iINSPIRE-00071410$$uBarcelona, IFAE 002007002 700__ $$aCasolino, Mirkoantonio$$iINSPIRE-00366594$$uBarcelona, IFAE 002007002 700__ $$aCastaneda-Miranda, Elizabeth$$iINSPIRE-00212108$$uJohannesburg U. 002007002 700__ $$aCastelli, Angelantonio$$iINSPIRE-00342579$$uFOM, Amsterdam 002007002 700__ $$aCastillo Gimenez, Victoria$$iINSPIRE-00212120$$uValencia U., IFIC 002007002 700__ $$aCastro, Nuno Filipe$$iINSPIRE-00036257$$uLIP, Lisbon$$uPorto U. 002007002 700__ $$aCatastini, Pierluigi$$iINSPIRE-00041380$$uHarvard U., Phys. 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London 002007002 700__ $$aChitan, Adrian$$iINSPIRE-00236054$$uBucharest, IFIN-HH 002007002 700__ $$aChizhov, Mihail$$iINSPIRE-00227239$$uDubna, JINR 002007002 700__ $$aChoi, Kyungeon$$iINSPIRE-00180982$$uIndiana U. 002007002 700__ $$aChouridou, Sofia$$iINSPIRE-00212583$$uAthens U. 002007002 700__ $$aChow, Bonnie Kar Bo$$iINSPIRE-00334326$$uMunich U. 002007002 700__ $$aChristodoulou, Valentinos$$iINSPIRE-00407394$$uUniversity Coll. London 002007002 700__ $$aChromek-Burckhart, Doris$$iINSPIRE-00305640$$uCERN 002007002 700__ $$aChu, Ming-Lee$$iINSPIRE-00226630$$uTaiwan, Inst. Phys. 002007002 700__ $$aChudoba, Jiri$$iINSPIRE-00150160$$uPrague, Inst. 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U. Navale 002007002 700__ $$aCooke, Mark$$iINSPIRE-00183948$$uLBL, Berkeley 002007002 700__ $$aCooper, Ben$$iINSPIRE-00041328$$uUniversity Coll. London 002007002 700__ $$aCooper-Sarkar, Amanda$$iINSPIRE-00074346$$uOxford U. 002007002 700__ $$aCornelissen, Thijs$$iINSPIRE-00212766$$uWuppertal U. 002007002 700__ $$aCorradi, Massimo$$iINSPIRE-00001854$$uINFN, Bologna 002007002 700__ $$aCorriveau, Francois$$iINSPIRE-00074601$$uMcGill U.$$uIPP, Canada 002007002 700__ $$aCorso-Radu, Alina$$iINSPIRE-00305712$$uUC, Irvine 002007002 700__ $$aCortes-Gonzalez, Arely$$iINSPIRE-00212778$$uBarcelona, IFAE 002007002 700__ $$aCortiana, Giorgio$$iINSPIRE-00041311$$uMunich, Max Planck Inst. 002007002 700__ $$aCosta, Giuseppe$$iINSPIRE-00212780$$uINFN, Milan 002007002 700__ $$aCosta, María José$$iINSPIRE-00212791$$uValencia U., IFIC 002007002 700__ $$aCostanzo, Davide$$iINSPIRE-00212803$$uSheffield U. 002007002 700__ $$aCôté, David$$iINSPIRE-00027694$$uTexas U., Arlington 002007002 700__ $$aCottin, Giovanna$$iINSPIRE-00334334$$uCambridge U. 002007002 700__ $$aCowan, Glen$$iINSPIRE-00145177$$uRoyal Holloway, U. of London 002007002 700__ $$aCox, Brian$$iINSPIRE-00074854$$uManchester U. 002007002 700__ $$aCranmer, Kyle$$iINSPIRE-00074922$$uNew York U. 002007002 700__ $$aCree, Graham$$iINSPIRE-00349746$$uCarleton U. 002007002 700__ $$aCrépé-Renaudin, Sabine$$iINSPIRE-00074993$$uLPSC, Grenoble 002007002 700__ $$aCrescioli, Francesco$$iINSPIRE-00030662$$uParis U., VI-VII 002007002 700__ $$aCribbs, Wayne Allen$$iINSPIRE-00360698$$uStockholm U.$$uStockholm U., OKC 002007002 700__ $$aCrispin Ortuzar, Mireia$$iINSPIRE-00339030$$uOxford U. 002007002 700__ $$aCristinziani, Markus$$iINSPIRE-00058643$$uBonn U. 002007002 700__ $$aCroft, Vince$$iINSPIRE-00366990$$uNIKHEF, Amsterdam 002007002 700__ $$aCrosetti, Giovanni$$iINSPIRE-00212870$$uINFN, Cosenza$$uCalabria U. 002007002 700__ $$aCuhadar Donszelmann, Tulay$$iINSPIRE-00043040$$uSheffield U. 002007002 700__ $$aCummings, Jane$$iINSPIRE-00329170$$uYale U. 002007002 700__ $$aCuratolo, Maria$$iINSPIRE-00212948$$uFrascati 002007002 700__ $$aCuthbert, Cameron$$iINSPIRE-00286420$$uSydney U. 002007002 700__ $$aCzirr, Hendrik$$iINSPIRE-00229786$$uSiegen U. 002007002 700__ $$aCzodrowski, Patrick$$iINSPIRE-00236101$$uAlberta U. 002007002 700__ $$aD'Auria, Saverio$$iINSPIRE-00212973$$uGlasgow U. 002007002 700__ $$aD'Onofrio, Monica$$iINSPIRE-00041292$$uLiverpool U. 002007002 700__ $$aDa Cunha Sargedas De Sousa, Mario Jose$$iINSPIRE-00339043$$uLIP, Lisbon$$uLisbon U., CFNUL 002007002 700__ $$aDa Via, Cinzia$$iINSPIRE-00212924$$uManchester U. 002007002 700__ $$aDabrowski, Wladyslaw$$iINSPIRE-00178895$$uAGH-UST, Cracow 002007002 700__ $$aDafinca, Alexandru$$iINSPIRE-00236119$$uOxford U. 002007002 700__ $$aDai, Tiesheng$$iINSPIRE-00212987$$uMichigan U. 002007002 700__ $$aDale, Orjan$$iINSPIRE-00358740$$uBergen U. 002007002 700__ $$aDallaire, Frederick$$iINSPIRE-00334341$$uMontreal U. 002007002 700__ $$aDallapiccola, Carlo$$iINSPIRE-00075606$$uMassachusetts U., Amherst 002007002 700__ $$aDam, Mogens$$iINSPIRE-00075612$$uBohr Inst. 002007002 700__ $$aDandoy, Jeffrey Rogers$$iINSPIRE-00396074$$uChicago U., EFI 002007002 700__ $$aDang, Nguyen Phuong$$iINSPIRE-00410760$$uFreiburg U. 002007002 700__ $$aDaniells, Andrew Christopher$$iINSPIRE-00338698$$uBirmingham U. 002007002 700__ $$aDanninger, Matthias$$iINSPIRE-00324867$$uBritish Columbia U. 002007002 700__ $$aDano Hoffmann, Maria$$iINSPIRE-00354223$$uIRFU, Saclay 002007002 700__ $$aDao, Valerio$$iINSPIRE-00213005$$uFreiburg U. 002007002 700__ $$aDarbo, Giovanni$$iINSPIRE-00213017$$uINFN, Genoa 002007002 700__ $$aDarmora, Smita$$iINSPIRE-00337045$$uTexas U., Arlington 002007002 700__ $$aDassoulas, James$$iINSPIRE-00286438$$uAlberta U. 002007002 700__ $$aDattagupta, Aparajita$$iINSPIRE-00221224$$uIndiana U. 002007002 700__ $$aDavey, Will$$iINSPIRE-00213030$$uBonn U. 002007002 700__ $$aDavid, Claire$$iINSPIRE-00342591$$uVictoria U. 002007002 700__ $$aDavidek, Tomas$$iINSPIRE-00075913$$uCharles U. 002007002 700__ $$aDavies, Eleanor$$iINSPIRE-00236121$$uOxford U.$$uRutherford 002007002 700__ $$aDavies, Merlin$$iINSPIRE-00213066$$uTel Aviv U. 002007002 700__ $$aDavison, Peter$$iINSPIRE-00345754$$uUniversity Coll. London 002007002 700__ $$aDavygora, Yuriy$$iINSPIRE-00236134$$uKirchhoff Inst. 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C$$v92$$y2015 002007002 8564_ $$uhttp://arxiv.org/pdf/1504.01289.pdf$$yPreprint 002007002 8564_ $$81079187$$s1713052$$uhttp://cds.cern.ch/record/2007002/files/arXiv:1504.01289.pdf 002007002 8564_ $$81079193$$s27352$$uhttp://cds.cern.ch/record/2007002/files/fig_05.png$$y00004 (Color online) The correlation of the $v_m$ between $0.5<\pT<2$~GeV ($x$-axis) and $3<\pT<4$~GeV ($y$-axis) for $m=2$ (left panel) and $m=3$ (right panel). The $v_m$ values are calculated for fourteen 5\% centrality intervals in the centrality range 0--70\% without event-shape selection. The data points are connected to show the boomerang trend from central to peripheral collisions as indicated. The error bars and shaded boxes represent the statistical and systematic uncertainties, respectively. These uncertainties are often smaller than the symbol size. 002007002 8564_ $$81079189$$s35948$$uhttp://cds.cern.ch/record/2007002/files/fig_01.png$$y00000 (Color online) The distributions of the magnitude of the flow vector, $q_2$ (left panel) and $q_3$ (right panel), calculated in the FCal via Eq.~(\ref{eq:1aa}) in the 1\% most central collisions. The vertical lines indicate the boundaries of the fifteen $q_m$ ranges, each containing a fraction of events as indicated. 002007002 8564_ $$81079196$$s40875$$uhttp://cds.cern.ch/record/2007002/files/fig_09.png$$y00008 (Color online) The correlation of $v_2$ ($x$-axis) with $v_4$ ($y$-axis) both measured in $0.5<\pT<2$ GeV. The left panel shows the $v_2$ and $v_4$ values for thirteen 5\% centrality intervals over the centrality range 0--65\% without event-shape selection. The data points are connected to show the boomerang trend from central to peripheral collisions as indicated. The right panel shows the $v_2$ and $v_4$ values in different $q_2$ intervals in seven centrality ranges (markers) with larger $v_2$ value corresponding to larger $q_2$ value; they are overlaid with the centrality dependence from the left panel. The error bars and shaded boxes represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81079190$$s44447$$uhttp://cds.cern.ch/record/2007002/files/fig_12.png$$y00011 (Color online) The correlation of $v_3$ ($x$-axis) with $v_4$ ($y$-axis) both measured in $0.5<\pT<2$ GeV. The left panel shows the $v_3$ and $v_4$ values in thirteen 5\% centrality intervals over the centrality range 0--65\% without event-shape selection. The data points are connected to show the boomerang trend from central to peripheral collisions as indicated. The right panel shows the $v_3$ and $v_4$ values for fourteen $q_3$ selections (the two highest $q_3$ intervals in Fig.~\ref{fig:0a} are combined) in several centrality ranges (markers) with larger $v_3$ value corresponding to larger $q_3$ value; they are overlaid with the centrality dependence from the left panel. The error bars and shaded boxes represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81079191$$s45032$$uhttp://cds.cern.ch/record/2007002/files/fig_07.png$$y00006 (Color online) The correlation of $v_2$ ($x$-axis) with $v_3$ ($y$-axis) both measured in $0.5<\pT<2$ GeV. The left panel shows the $v_2$ and $v_3$ values for fourteen 5\% centrality intervals over the centrality range 0--70\% without event-shape selection. The data points are connected to show the boomerang trend from central to peripheral collisions as indicated. The right panel shows the $v_2$ and $v_3$ values in the fifteen $q_2$ intervals in seven centrality ranges (markers) with larger $v_2$ value corresponding to larger $q_2$ value; they are overlaid with the centrality dependence from the left panel. The error bars and shaded boxes represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81079188$$s46984$$uhttp://cds.cern.ch/record/2007002/files/fig_02.png$$y00001 (Color online) The correlation functions $C(\Delta\phi)$ for pairs with $|\Delta\eta|>2$ and $0.5<\pT<2$~GeV in 0--5\% centrality. The correlation functions for events with the largest 10\% and smallest 10\% $q_m$ values are also shown for $m=2$ (left panel) and $m=3$ (right panel). The statistical uncertainties are smaller than the symbols. 002007002 8564_ $$81079195$$s51806$$uhttp://cds.cern.ch/record/2007002/files/fig_11.png$$y00010 (Color online) The centrality ($\npart$) dependence of the $v_4$ in $0.5<\pT<2$~GeV and the associated linear and nonlinear components extracted from the fits in Fig.~\ref{fig:3c} and Eq.~(\ref{eq:2c}). They are compared with the linear and nonlinear component estimated from the previously published event-plane correlations~\cite{Aad:2014fla} via Eq.~(\ref{eq:2d}). The error bars represent the statistical uncertainties, while the shaded bands or hashed bands represent the systematic uncertainties. 002007002 8564_ $$81079200$$s53250$$uhttp://cds.cern.ch/record/2007002/files/fig_15a.png$$y00014 (Color online) The centrality ($\npart$) dependence of the $v_5$ in $0.5<\pT<2$~GeV and the associated linear and nonlinear components extracted from the fits in Fig.~\ref{fig:4c}, Fig.~\ref{fig:4cc} and Eq.~(\ref{eq:2f}). They are compared with the linear and nonlinear component estimated from the previous published event-plane correlation~\cite{Aad:2014fla} via Eq.~(\ref{eq:2g}). The error bars represent the statistical uncertainties, while the shaded bands or hashed bands represent the systematic uncertainties. 002007002 8564_ $$81079192$$s60453$$uhttp://cds.cern.ch/record/2007002/files/fig_04a.png$$y00003 (Color online) The correlations between $v_n$ and $q_2$ (left column) and $q_3$ (right column) in four centrality intervals with $n=2$ (top row), $n=3$ (second row), $n=4$ (third row) and $n=5$ (bottom row), where $v_n$ is calculated in $0.5<\pT<2$~GeV. Only statistical uncertainties are shown. The lines connecting data points are for guidance only. 002007002 8564_ $$81079198$$s63559$$uhttp://cds.cern.ch/record/2007002/files/fig_16.png$$y00015 (Color online) The eccentricity-scaled $v_n$ or the estimated linear component $v_n^{\rm L}$ obtained from two-component fits, $v_2/\sqrt{\langle\epsilon_2^2\rangle}$ (circles), $v_3/\sqrt{\langle\epsilon_3^2\rangle}$ (boxes), $v_4^{\rm L}/\sqrt{\langle\epsilon_4^2\rangle}$ (solid diamonds), $v_5^{\rm L}/\sqrt{\langle\epsilon_5^2\rangle}$ (solid crosses), $v_4/\sqrt{\langle\epsilon_4^2\rangle}$ (open diamonds), and $v_5/\sqrt{\langle\epsilon_5^2\rangle}$ (open crosses). The eccentricities are calculated from the MC Glauber model (left panel) and the MC-KLN model (right panel). The error bars represent the statistical uncertainties, while the shaded bands or hashed bands represent the systematic uncertainties. 002007002 8564_ $$81079201$$s72079$$uhttp://cds.cern.ch/record/2007002/files/fig_03a.png$$y00002 (Color online) The harmonic flow coefficients $v_n(\pT)$ in the 20--30\% centrality interval for events selected on either $q_2$ (left column) or $q_3$ (right column) for $n=2$ (top row), $n=3$ (second row), $n=4$ (third row) and $n=5$ (bottom row). They are calculated for reference $\pT$ of $0.5<\ptb <2$~GeV [Eq.~(\ref{eq:1f})]. The top part of each panel shows the $v_n(\pT)$ for events in the 0--0.1, 0.1--0.2, 0.7--0.8 and 0.9--1 fractional ranges of $q_m$ (open symbols) as well as for inclusive events without $q_m$ selection (solid symbols). The bottom part of each panel shows the ratios of the $v_n(\pT)$ for $q_m$-selected events to those obtained for all events. Only statistical uncertainties are shown. 002007002 8564_ $$81079203$$s74610$$uhttp://cds.cern.ch/record/2007002/files/fig_06.png$$y00005 (Color online) The correlation of $v_m$ between the $0.5<\pT<2$~GeV ($x$-axis) and $3<\pT<4$~GeV range ($y$-axis) for $m=2$ (left panel) and $m=3$ (right panel) in various centrality intervals. The data points are calculated in various $q_m$ intervals defined in Fig.~\ref{fig:0a} for each centrality, and they increase monotonically with increasing $q_m$ value. These data are overlaid with the centrality dependence without $q_m$ selection from Fig.~\ref{fig:1}. The thin solid straight lines represent a linear fit of the data in each centrality interval, and error bars represent the statistical uncertainties. 002007002 8564_ $$81079194$$s80380$$uhttp://cds.cern.ch/record/2007002/files/fig_13.png$$y00012 (Color online) The correlation of $v_2$ ($x$-axis) with $v_5$ ($y$-axis) in $0.5<\pT<2$~GeV for fourteen $q_2$ selections (the two highest $q_2$ intervals in Fig.~\ref{fig:0a} are combined) in nine 5\% centrality intervals. The data are compared with the rescaled $\epsilon_2$--$\epsilon_5$ correlation from MC Glauber and MC-KLN models in the same centrality interval. The data are also parameterized with Eq.~(\ref{eq:2e}), taking into account both statistical and systematic uncertainties. The $\npart$ dependence of the fit parameters is shown in the last two panels. The error bars and shaded bands represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81079199$$s81479$$uhttp://cds.cern.ch/record/2007002/files/fig_14.png$$y00013 (Color online) The correlation of $v_3$ ($x$-axis) with $v_5$ ($y$-axis) in $0.5<\pT<2$~GeV for fourteen $q_3$ selections (the two highest $q_3$ intervals in Fig.~\ref{fig:0a} are combined) in nine 5\% centrality intervals. The data are compared with the rescaled $\epsilon_3$--$\epsilon_5$ correlation from MC Glauber and MC-KLN models in the same centrality interval. The data are also parameterized with Eq.~(\ref{eq:2e}), taking into account both statistical and systematic uncertainties. The $\npart$ dependence of the fit parameters is shown in the last two panels. The error bars and shaded bands represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81079197$$s91892$$uhttp://cds.cern.ch/record/2007002/files/fig_08.png$$y00007 (Color online) The correlation of $v_2$ ($x$-axis) with $v_3$ ($y$-axis) in $0.5<\pT<2$~GeV for fifteen $q_2$ selections in thirteen 5\% centrality intervals. The data are compared with the rescaled $\epsilon_2$--$\epsilon_3$ correlation from MC Glauber and MC-KLN models in the same centrality interval. The data are also parameterized with a linear function [Eq.~(\ref{eq:2a})], taking into account both the statistical and systematic uncertainties. The $\npart$ dependence of the fit parameters is shown in the last two panels. The error bars and shaded bands represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81079202$$s99221$$uhttp://cds.cern.ch/record/2007002/files/fig_10.png$$y00009 (Color online) The correlation of $v_2$ ($x$-axis) with $v_4$ ($y$-axis) in $0.5<\pT<2$~GeV for fifteen $q_2$ selections in thirteen 5\% centrality intervals. The data are compared with the rescaled $\epsilon_2$--$\epsilon_4$ correlation from MC Glauber and MC-KLN models in the same centrality interval. The data are also parameterized with Eq.~(\ref{eq:2b}), taking into account both statistical and systematic uncertainties. The $\npart$ dependence of the fit parameters is shown in the last two panels. The error bars and shaded bands represent the statistical and systematic uncertainties, respectively. 002007002 8564_ $$81192208$$s1729020$$uhttp://cds.cern.ch/record/2007002/files/PhysRevC.92.pdf 002007002 916__ $$sn$$w201514 002007002 960__ $$a13 002007002 980__ $$aARTICLE 002007002 980__ $$aCERN 002007002 980__ $$aATLAS_Papers