REVIEW
J/Psi Elliptic Flow in Pb-Pb Collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
Nuclear Experiment · Submitted 23 Mar 2013 · 28 references
Pith's verdict: First J/ψ v2 at the LHC, honestly labeled a 2.7–2.9σ indication; the background-shape systematic is the real soft spot, and the paper handles it about as well as these data allow.
T0 · AI review
Why Pith says this
Highlight any text to comment on it.
Referee report
The paper
The paper claims
ALICE reports the first measurement of J/ψ elliptic flow in Pb-Pb collisions at the LHC, finding a 2.7σ indication that the meson's azimuthal anisotropy is non-zero at intermediate transverse momentum.
The reading
What carries the argument
The measurement rests on two pieces of machinery. The first is the event-plane method: the second-harmonic plane angle $Ψ$ is reconstructed from the VZERO-A scintillator array only, deliberately excluding VZERO-C because it overlaps in acceptance with the muon spectrometer and would introduce autocorrelations; the resulting resolution, from 0.185 in the 60%–90% class to 0.610 in 20%–40%, is corrected for and carries a 1.3% correlated systematic. The second is the fit of $v_2$ as a function of dimuon invariant mass, $v_2(m_{μμ}) = v_2^{sig} α(m_{μμ}) + v_2^{bkg}(m_{μμ})[1 - α(m_{μμ})]$, in which the signal fraction $α = S/(S+B)$ comes from a Crystal Ball plus continuum fit to the opposite-sign mass spectrum and $v_2^{bkg}$ is parametrized by a polynomial. The physics mechanism the numbers are weighed against is the competition between primordial J/ψ, which acquire only a small anisotropy from in-plane versus out-of-plane path lengths, and regenerated J/ψ, which inherit the full elliptic flow of thermalized charm quarks.
Extended reading notes
Core claim
The paper reports the first measurement of inclusive J/ψ elliptic flow in heavy-ion collisions at the LHC, using $17$ million dimuon-triggered Pb-Pb events at $2.76$ TeV in the rapidity range $2.5 < y < 4.0$. The elliptic flow is extracted as $v_2 = 2.7$–$2.9$σ non-zero in semi-central collisions: $v_2 = 0.116$ for $2 < p_T < 4$ GeV/$c$ in the 20%–40% class, with the broader $1.5 < p_T < 10$ GeV/$c$ sample giving $0.101$ (5%–20%) and $0.116$ (20%–40%). Peripheral collisions (40%–60% and 60%–90%) are consistent with zero, and the reconstructed mean transverse momentum stays in the narrow band 3.0–3.3 GeV/$c$ across centralities, so the centrality trend is not a $p_T$ migration artefact. The authors read this pattern as favouring a regeneration component: transport calculations in which about 30% of the observed J/ψ in the 20%–60% range come from deconfined charm quarks reproduce both the shape of $v_2(p_T)$ and the previously published nuclear modification factor, whereas a purely primordial population would give $v_2$ near 0.02 at $p_T ≈ 2.5$ GeV/$c$.
Load-bearing premise
The extraction assumes that the azimuthal anisotropy of the dimuon background as a function of invariant mass is captured by the three parametrizations tried, a second-order polynomial, a first-order polynomial and its inverse, and that the largest spread among them is a conservative enough systematic; the authors themselves identify this background-shape uncertainty as the dominant one, so a true background anisotropy outside that family would shift the fitted signal and move the significance with it.
Editorial extensions
If this is right
- The inclusive J/ψ nuclear modification factor measured earlier by ALICE, which is larger than at RHIC and shows no strong centrality dependence, gains a companion observable that points the same way: low-$p_T$ J/ψ are not simply the survivors of suppression.
- Charm quarks must be substantially thermalized in the medium at LHC energies, since regeneration can only transfer flow that the charm quarks themselves carry.
- The qualitative difference from the STAR measurement at $\sqrt{s_{NN}} = 200$ GeV, which is compatible with zero for $p_T \geq 2$ GeV/$c$, becomes a genuine energy dependence of the charm-sector dynamics rather than a statistical fluctuation.
- Transport models with regeneration, which already described the nuclear modification factor, are now constrained on a second, independent axis and survive that test.
- Non-prompt J/ψ from b-hadron decays, at roughly 7%–11% of the sample, could themselves carry flow if bottom quarks thermalize, so the measured value is a lower bound on the prompt component's anisotropy under that hypothesis.
Reading between the lines
- If the effect is real, the natural next discriminant is the $p_T$ at which $v_2$ turns over: regeneration models place the maximum near $2.5$ GeV/$c$ because primordial J/ψ take over above it, so a measured turnover position that moves with centrality would be hard to accommodate without tuning the regeneration fraction.
- The same event-plane machinery applied to the $\Upsilon$ family would test whether the mechanism scales with quark mass as thermalization arguments suggest, since bottom quarks are heavier and are expected to flow less at a given $p_T$.
- A data-driven continuum anisotropy, taken from same-sign dimuons rather than from a fitted polynomial family, would shrink the dominant systematic and could turn a 2.7σ indication into a measurement; the paper already notes that same-sign pairs follow the opposite-sign continuum trend.
- Because the flow is inherited rather than generated by the J/ψ itself, a correlated measurement of open-charm $D$-meson $v_2$ in the same centrality and $p_T$ bins would either confirm a common parent anisotropy or expose a mismatch that regeneration alone cannot explain.
Original abstract
We report on the first measurement of inclusive J/$\psi$ elliptic flow, $v_2$, in heavy-ion collisions at the LHC. The measurement is performed with the ALICE detector in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV in the rapidity range $2.5 < y < 4.0$. The dependence of the J/$\psi$ $v_2$ on the collision centrality and on the J/$\psi$ transverse momentum is studied in the range $0 < p_{\rm T} < 10$ GeV/$c$. For semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV, an indication of non-zero $v_2$ is observed with a maximum value of $v_2 = 0.116 \pm 0.046 {\rm (stat.)} \pm 0.029 {\rm (syst.)}$ for J/$\psi$ in the transverse momentum range $2 < p_{\rm T} < 4$ GeV/$c$. The elliptic flow measurement complements the previously reported ALICE results on the inclusive J/$\psi$ nuclear modification factor and favors the scenario of a significant fraction of J/$\psi$ production from charm quarks in a deconfined partonic phase.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
We report on the first measurement of inclusive J/$\psi$ elliptic flow, $v_2$, in heavy-ion collisions at the LHC. The measurement is performed with the ALICE detector in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV in the rapidity range $2.5 < y < 4.0$. The dependence of the J/$\psi$ $v_2$ on the collision centrality and on the J/$\psi$ transverse momentum is studied in the range $0 < p_{\rm T} < 10$ GeV/$c$. For semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV, an indication of non-zero $v_2$ is observed with a maximum value of $v_2 = 0.116 \pm 0.046 {\rm (stat.)} \pm 0.029 {\rm (syst.)}$ for J/$\psi$ in the transverse momentum range $2 < p_{\rm T} < 4$ GeV/$c$. The elliptic flow measurement complements the previously reported ALICE results on the inclusive J/$\psi$ nuclear modification factor and favors the scenario of a significant fraction of J/$\psi$ production from charm quarks in a deconfined partonic phase.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We report on the first measurement of inclusive J/$\psi$ elliptic flow, $v_2$, in heavy-ion collisions at the LHC. | contribution 1.00 | 0.97 | 0.11 | asserted 0.99 |
| s1 | The measurement is performed with the ALICE detector in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV in the rapidity range $2.5 < y < 4.0$. | method 0.99 | 0.94 | 0.02 | asserted 1.00 |
| s2 | The dependence of the J/$\psi$ $v_2$ on the collision centrality and on the J/$\psi$ transverse momentum is studied in the range $0 < p_{\rm T} < 10$ GeV/$c$. | contribution 0.62 | 0.89 | 0.03 | asserted 0.93 |
| s3 | For semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV, an indication of non-zero $v_2$ is observed with a maximum value of $v_2 = 0.116 \pm 0.046 {\rm (stat.)} \pm 0.029 {\rm (syst.)}$ for J/$\psi$ in the transverse momentum range $2 < p_{\rm T} < 4$ GeV/$c$. | result 1.00 | 0.97 | 0.44 | hedged possibility 0.94 |
| s4 | The elliptic flow measurement complements the previously reported ALICE results on the inclusive J/$\psi$ nuclear modification factor and favors the scenario of a significant fraction of J/$\psi$ production from charm quarks in a deconfined partonic phase. | interpretation 1.00 | 0.59 | 0.74 | hedged possibility 0.62 |
What was examined, and what was not
- arXiv listing abstract v4
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
Figures
Figures reproduced from arXiv:1303.5880 by the authors.
References
How later papers used it
48 later papers cite it
1 paper by the same authors is listed below: 1 compared its own results with it.
Compares with it 1 of 4 papers with this label · 1 by the same authors
By the same authors
-
The transport models considered in this paper are also able to generate an amount of elliptic flow comparable to the one measured in ALICE [ref] .
Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV (2015) (same authors) · Conclusions · 0.80
How the literature uses it
46 arXiv papers cite this in 51 sentences
Papers whose main result relates to this one's
States the same result 1 paper
-
We present the first inclusive J/psi elliptic flow measurement performed with the muon spectrometer of ALICE, in Pb-Pb collisions, at forward rapidity.
Papers citing it · 40 sentences without a confident label
Uses its method or tool 1 paper
-
In both and collisions, the $v_2(Δφ, Δη)$ can be written [ref] as the weighted sum of the $v_2$ of jet particles ($v_2^jet part$) and background ($v_2^B(Δφ)$), as [equation] where the jet-particle $S(Δφ, Δη)$ and background $B(Δφ, Δη)$ yields are extracted from the two-particle correlation functions constructed in the TPC.
Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV · Introduction · 0.85
Uses its data or values 1 paper
-
ALICE measured a non-zero for inclusive in semi-central collisions at forward rapidity [ref] in the range 2 $<$ $<$6 GeV/$c$.
An overview of experimental results from ultra-relativistic heavy-ion collisions at the CERN LHC: hard probes · Quarkonia · 0.80
Compares with it 3 papers
-
The first such result, for $$ elliptic flow $v_2(p_T)$, is shown in Fig. [ref] and compared with experimental data for $v_2$ of $J/Ψ$ and $D$ mesons [ref] .
Deciphering the nature of X(3872) in heavy ion collisions · Introduction · 0.98
-
The transport models considered in this paper are also able to generate an amount of elliptic flow comparable to the one measured in ALICE [ref] .
Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV · Conclusions · 0.80
-
This affirms well with the results at $√(s_NN) = 2.76$ TeV [ref] in semi-central collisions.
Anisotropic flow: A case for Bottomonia · Charmonia Flow · 0.92
Cites it as support 3 papers
-
A strong indication for equilibration is the fact that J/$ψ$ mesons participate in the collective, anisotropic hydrodynamic expansion [ref] .
QCD under extreme conditions · Section · 0.98
-
In addition, the indication of a non-zero elliptic flow in collisions at 2.76 observed by ALICE [ref] brings another hint in favor of (re)combination scenarios.
Centrality, rapidity and transverse momentum dependence of $J/\psi$ suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=2.76 TeV · Conclusions · 0.96
-
A strong indication for equilibration is the fact that J/$ψ$ mesons participate in the collective, anisotropic hydrodynamic expansion [ref] .
Statistical hadronization: successes and some open issues · Extension to hadrons with heavy quarks · 0.96
Cites it as background 3 papers
-
Heavy quarkonium states in and collisions were mainly studied by ALICE [ref] and CMS [ref] , with contributions on selected topics also from ATLAS [ref] and LHCb [ref] .
Heavy-ion collisions at the Large Hadron Collider: a review of the results from Run 1 · Quarkonium · 0.80
-
Measurements related heavy quark production [ref] , dilepton production, jet-hadron correlations [ref] and higher order azimuthal anisotropy [ref] which are now coming out of both RHIC and LHC experiments will provide a much more detail characterization of the properties of the QCD matter formed in heavy-ion collisions.
Selected Experimental Results from Heavy Ion Collisions at LHC · Summary · 0.84
-
Large amount of data on charmonium and bottomonium production is available at RHIC [ref] and at the LHC [ref] significantly extending our understanding of quarkonium production in deconfined matter [ref] .
Status of quarkonia - like negative and positive parity states in a relativistic confinement scheme · Introduction · 0.87
What it cites · 10 sentences without a confident label
Uses the method or tool of 6 papers
-
The ȷ$v_2$ results were obtained determining $v_2 = ⟨cos2 (ϕ- Ψ) ⟩$ versus the invariant mass ($m_μμ$) [ref] , where $ϕ$ is the OS dimuon azimuthal angle.
Azimuthally sensitive correlations in nucleus-nucleus collisions · Introduction · 1.00
-
The azimuthal angle $Ψ$ of the second harmonic EP is used to estimate the reaction plane angle [ref] . $Ψ$ is determined from the azimuthal distribution of the VZERO amplitude.
Methods for analyzing anisotropic flow in relativistic nuclear collisions · Introduction · 1.00
-
A two step flattening procedure of the EP azimuthal distribution was applied as described in [ref] and [ref] , respectively.
Proton and Pion Production Relative to the Reaction Plane in Au + Au Collisions at AGS Energies · Introduction · 1.00
Uses data or values from 1 paper
-
The LHCb Collaboration measured the fraction of ȷfrom B hadron decays in pp collisions at $√(s)$ = 2.76 and 7 TeV [ref] in the rapidity acceptance used for this measurement.
Measurement of J/psi production in pp collisions at sqrt(s)=2.76 TeV · Introduction · 0.82
Compares with 2 papers
-
This trend seems qualitatively different from that of the STAR measurement [ref] at lower collision energy, which is compatible with zero for $p_T ≥2$ GeV/$c$ albeit in somewhat different (10%–40% and 0%–80%) centrality ranges.
Measurement of J/{psi} Azimuthal Anisotropy in Au+Au Collisions at {sqrt{s_{NN}}} = 200 GeV · Introduction · 1.00
-
The inclusive ȷ reported is larger than that measured at the SPS [ref] and at RHIC [ref] for central collisions and does not exhibit a significant centrality dependence.
1103.6269 · Introduction · 0.99
Cites as background 1 paper
-
Quarkonia (a heavy quark and anti-quark bound state) are therefore expected to be sensitive to the properties of the strongly-interacting system formed in the early stages of heavy-ion collisions [ref] .
Hard probes in heavy ion collisions at the LHC: heavy flavour physics · Introduction · 0.91
Discussion
Disagree with the review, or know something it missed? Leave a comment, highlight any passage above to comment on it, or challenge this review formally.