We prese
nt measureme
nts of the elliptic (
n id="mmlsi2" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si2.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=9ca06101309bad52b1ff201bcbd21958" title="Click to view the MathML source">v2n>n class="mathContainer hidden">n class="mathCode">n>n>n>), tria
ngular (
n id="mmlsi3" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si3.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=4285627d45ccdda4c0d45ff7ed4a256b" title="Click to view the MathML source">v3n>n class="mathContainer hidden">n class="mathCode">n>n>n>) a
nd quadra
ngular (
n id="mmlsi4" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si4.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=afabd775fa7380dd028f231d672a093d" title="Click to view the MathML source">v4n>n class="mathContainer hidden">n class="mathCode">n>n>n>) a
nisotropic azimuthal flow over a wide ra
nge of pseudorapidities (
n id="mmlsi5" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si5.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=8a85b44dae8fb199e19945be549092d8" title="Click to view the MathML source">−3.5<η<5n>n class="mathContainer hidden">n class="mathCode">n>n>n>). The measureme
nts are performed with Pb&
ndash;Pb collisio
ns at
n id="mmlsi1" class="mathmlsrc">nce?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si1.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=d8ce3f723832d73f2f75919ffd39233c">nlineImage" height="15" width="105" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316303586-si1.gif"><noscript>n:bottom" width="105" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0370269316303586-si1.gif">noscript>n class="mathContainer hidden">n class="mathCode">n>n>n> usi
ng the ALICE detector at the Large Hadro
n Collider (LHC). The flow harmo
nics are obtai
ned usi
ng two- a
nd four-particle correlatio
ns from
ni
ne differe
nt ce
ntrality i
ntervals coveri
ng ce
ntral to peripheral collisio
ns. We fi
nd that the shape of
n id="mmlsi6" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si6.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=75251f1f46549c175e779ff2b4ae8a8d" title="Click to view the MathML source">vn(η)n>n class="mathContainer hidden">n class="mathCode">n>n>n> is largely i
ndepe
nde
nt of ce
ntrality for the flow harmo
nics
n id="mmlsi7" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si7.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=ea9a291dd8beedf88a13c9103c79334a" title="Click to view the MathML source">n=2–4n>n class="mathContainer hidden">n class="mathCode">n>n>n>, however the higher harmo
nics fall off more steeply with i
ncreasi
ng
n id="mmlsi8" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si8.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=8f072ec63cf8a21187020234d0a227ae" title="Click to view the MathML source">|η|n>n class="mathContainer hidden">n class="mathCode">n>n>n>. We assess the validity of exte
nded lo
ngitudi
nal scali
ng of
n id="mmlsi2" class="mathmlsrc">n class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303586&_mathId=si2.gif&_user=111111111&_pii=S0370269316303586&_rdoc=1&_issn=03702693&md5=9ca06101309bad52b1ff201bcbd21958" title="Click to view the MathML source">v2n>n class="mathContainer hidden">n class="mathCode">n>n>n> by compari
ng to lower e
nergy measureme
nts, a
nd fi
nd that the higher harmo
nic flow coefficie
nts are proportio
nal to the charged particle de
nsities at larger pseudorapidities. Fi
nally, we compare our measureme
nts to both hydrody
namical a
nd tra
nsport models, a
nd fi
nd they both have challe
nges whe
n it comes to describi
ng our data.