pith. sign in

arxiv: 2411.12101 · v2 · pith:GDPEBA6Dnew · submitted 2024-11-18 · ⚛️ nucl-ex

Beam-energy dependence of correlations between mean transverse momentum and anisotropic flow of charged particles in Au+Au collisions at RHIC

Pith reviewed 2026-05-23 16:44 UTC · model grok-4.3

classification ⚛️ nucl-ex
keywords heavy-ion collisionsanisotropic flowtransverse momentum correlationsbeam energy dependenceSTAR experimentshear viscosityinitial state fluctuationsAu+Au collisions
0
0 comments X

The pith

Measurements reveal energy-dependent variances but similar dimensionless ratios for mean transverse momentum and anisotropic flow across RHIC beam energies.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper measures event-by-event correlations between the mean transverse momentum [pT] and the squared anisotropic flow v_n^2 in Au+Au collisions at beam energies from 14.6 to 200 GeV. It finds that the variances and covariances of these quantities vary with beam energy, but their dimensionless ratio remains similar across the range. This is compared to hydrodynamic models and LHC data to gain insights into the specific shear viscosity and initial-state fluctuations in heavy-ion collisions.

Core claim

Our measurements reveal a distinct energy-dependent behavior in the variances and covariances. In addition, the dimensionless ratio displays a similar behavior across different beam energies.

What carries the argument

The dimensionless ratio of the variances and covariance of [pT] and v_n^2, which isolates effects from initial conditions and shear viscosity.

If this is right

  • These measurements can differentiate between different initial-state models in heavy-ion collisions.
  • The findings provide insights into the beam energy dependence of the specific shear viscosity eta/s.
  • Similar behavior of the ratio across energies suggests universal aspects in the correlation mechanism.
  • Comparisons with Pb+Pb at LHC help understand the energy evolution of these effects.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The consistent ratio might indicate that initial-state fluctuations scale in a particular way with energy that compensates for changes in viscosity.
  • Future measurements at even lower or higher energies could test if this similarity persists or breaks at phase transition points.
  • Improved hydrodynamic simulations without parameter tuning could be validated against these data points.

Load-bearing premise

Hydrodynamic models correctly capture the beam-energy dependence of both initial-state fluctuations and the specific shear viscosity without additional free parameters tuned to these observables.

What would settle it

A hydrodynamic model prediction that matches the energy dependence of variances but fails to reproduce the similar ratio across energies, or vice versa, would challenge the interpretation.

Figures

Figures reproduced from arXiv: 2411.12101 by The STAR Collaboration.

Figure 1
Figure 1. Figure 1: Comparison of the centrality dependence of (a) [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Comparison of the centrality dependence of (a) [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: The centrality dependence of the Var(v 2 3 )dyn (a), Ck (b), Cov(v 2 3 , [pT ]) (c), and ρ(v 2 3 , [pT ]) (d), for Au+Au collisions at √sNN = 200 and 54.4 GeV. The curve represents the LHC measurements [83]. The centrality and beam-energy dependence of Var(v 2 3 )dyn (a), Ck (b), Cov(v 2 3 , [pT ]) (c), and ρ(v 2 3 , [pT ]) (d) are presented in [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
read the original abstract

The correlation between the mean transverse momentum, $[p_{\mathrm{T}}]$, and the squared anisotropic flow, $v^{2}_{n}$, on an event-by-event basis has been suggested to be influenced by the initial conditions in heavy-ion collisions. We present measurements of the variances and covariance of $[p_{\mathrm{T}}]$ and $v^{2}_{n}$, along with their dimensionless ratio, for Au+Au collisions at various beam energies: $\sqrt{\textit{s}_{NN}}$ $=$ 14.6, 19.6, 27, 54.4, and 200~GeV. Our measurements reveal a distinct energy-dependent behavior in the variances and covariances. In addition, the dimensionless ratio displays a similar behavior across different beam energies. We compare our measurements with hydrodynamic models and similar measurements from Pb+Pb collisions at the Large Hadron Collider (LHC). These findings provide valuable insights into the beam energy dependence of the specific shear viscosity ($\eta/s$) and initial-state effects, allowing for differentiating between different initial-state models.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. The paper reports measurements of the variances and covariance of event-by-event mean transverse momentum [p_T] and squared anisotropic flow v_n^2, along with their dimensionless ratio, for Au+Au collisions at RHIC beam energies √s_NN = 14.6, 19.6, 27, 54.4, and 200 GeV. It finds distinct energy dependence in the variances and covariances but similar behavior in the ratio across energies, and compares the results to hydrodynamic models and LHC Pb+Pb data to constrain η/s and initial-state effects.

Significance. If the measurements are robust, they supply new experimental constraints on the beam-energy evolution of initial-state fluctuations and specific shear viscosity in heavy-ion collisions, helping discriminate among initial-state models.

minor comments (2)
  1. [Abstract] The abstract does not specify the centrality range or the method used to define centrality; adding this would clarify the kinematic domain of the reported energy dependence.
  2. Notation for the dimensionless ratio is introduced without an explicit equation; including its definition (e.g., as cov([p_T],v_n^2)/sqrt(var([p_T])var(v_n^2))) in the main text would improve readability.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the careful reading and positive assessment of our manuscript, including the recommendation for minor revision. The referee's summary accurately reflects the scope and findings of the work. No specific major comments were raised in the report.

Circularity Check

0 steps flagged

No significant circularity identified

full rationale

The paper reports direct experimental measurements of variances, covariances, and the dimensionless ratio of [p_T] and v_n^2 from Au+Au collision data at multiple RHIC energies. No derivation chain, first-principles prediction, or ansatz is claimed that reduces by construction to fitted inputs or self-citations. Model comparisons are external and interpretive only; the central claims are observational statements from data analysis and remain self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

This is an experimental measurement paper. The central claim rests on standard detector calibration, track reconstruction, and flow analysis procedures that are treated as established in the field rather than derived here. No new free parameters, axioms, or invented entities are introduced in the abstract.

pith-pipeline@v0.9.0 · 5717 in / 1153 out tokens · 23727 ms · 2026-05-23T16:44:13.974372+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

86 extracted references · 86 canonical work pages · 44 internal anchors

  1. [1]

    J. Adams, et al., Experimental and theoretical chal- lenges in the search for the quark gluon plasma: The STAR Collaboration’s critical assessment of the evidence from RHIC collisions, Nucl. Phys. A 757 (2005) 102–183. arXiv:nucl-ex/0501009, doi:10.1016/j.nuclphysa.2005.03.085

  2. [2]

    Formation of dense partonic matter in relativistic nucleus-nucleus collisions at RHIC: Experimental evaluation by the PHENIX collaboration

    K. Adcox, et al., Formation of dense partonic matter in relativistic nucleus-nucleus collisions at RHIC: Experi- mental evaluation by the PHENIX collaboration, Nucl. Phys. A 757 (2005) 184–283. arXiv:nucl-ex/0410003, doi:10.1016/j.nuclphysa.2005.03.086

  3. [3]

    Arsene, et al., Quark gluon plasma and color glass condensate at RHIC? The Perspective from the BRAHMS experiment, Nucl

    I. Arsene, et al., Quark gluon plasma and color glass condensate at RHIC? The Perspective from the BRAHMS experiment, Nucl. Phys. A 757 (2005) 1–27. arXiv:nucl-ex/0410020, doi:10.1016/j.nuclphysa.2005.02.130

  4. [4]

    B. B. Back, et al., The PHOBOS perspec- tive on discoveries at RHIC, Nucl. Phys. A 757 (2005) 28–101. arXiv:nucl-ex/0410022, doi:10.1016/j.nuclphysa.2005.03.084

  5. [5]

    First Results from Pb+Pb collisions at the LHC

    B. Muller, J. Schukraft, B. Wyslouch, First Re- sults from Pb+Pb collisions at the LHC, Ann. Rev. Nucl. Part. Sci. 62 (2012) 361–386. arXiv:1202.3233, doi:10.1146/annurev-nucl-102711-094910

  6. [6]

    E. V. Shuryak, Quark-Gluon Plasma and Hadronic Production of Leptons, Photons and Psions, Sov. J. Nucl. Phys. 28 (1978) 408. doi:10.1016/0370-2693(78)90370-2

  7. [7]

    E. V. Shuryak, Quantum Chromodynamics and the Theory of Superdense Matter, Phys. Rept. 61 (1980) 71–158. doi:10.1016/0370-1573(80)90105-2

  8. [8]

    Why does the Quark-Gluon Plasma at RHIC behave as a nearly ideal fluid ?

    E. Shuryak, Why does the quark gluon plasma at RHIC behave as a nearly ideal fluid?, Prog. Part. Nucl. Phys. 53 (2004) 273–303. arXiv:hep-ph/0312227, doi:10.1016/j.ppnp.2004.02.025

  9. [9]

    Conformal Relativistic Viscous Hydrodynamics: Applications to RHIC results at sqrt(s_NN) = 200 GeV

    M. Luzum, P. Romatschke, Conformal Rel- ativistic Viscous Hydrodynamics: Applica- tions to RHIC results at √ SN N = 200-GeV, Phys.Rev. C78 (2008) 034915. arXiv:0804.4015, doi:10.1103/PhysRevC.78.034915,10.1103/PhysRevC.79.039903

  10. [10]

    Bulk and shear viscosities of matter created in relativistic heavy-ion collisions

    P. Bozek, Bulk and shear viscosities of matter created in relativistic heavy-ion collisions, Phys. Rev. C 81 (2010) 034909. arXiv:0911.2397, doi:10.1103/PhysRevC.81.034909

  11. [11]

    Disappearance of Elliptic Flow: A New Probe for the Nuclear Equation of State

    P. Danielewicz, R. A. Lacey, P. Gossiaux, C. Pinken- burg, P. Chung, J. Alexander, R. McGrath, Dis- appearance of elliptic flow: a new probe for 5 the nuclear equation of state, Phys. Rev. Lett. 81 (1998) 2438–2441. arXiv:nucl-th/9803047, doi:10.1103/PhysRevLett.81.2438

  12. [12]

    U. W. Heinz, P. F. Kolb, Early ther- malization at RHIC, Nucl. Phys. A702 (2002) 269–280. arXiv:hep-ph/0111075, doi:10.1016/S0375-9474(02)00714-5

  13. [13]

    Hadronic dissipative effects on elliptic flow in ultrarelativistic heavy-ion collisions

    T. Hirano, U. W. Heinz, D. Kharzeev, R. Lacey, Y. Nara, Hadronic dissipative effects on elliptic flow in ultrarelativistic heavy-ion collisions, Phys.Lett. B636 (2006) 299–304. arXiv:nucl-th/0511046, doi:10.1016/j.physletb.2006.03.060

  14. [14]

    Huovinen, P

    P. Huovinen, P. F. Kolb, U. W. Heinz, P. V. Ruuskanen, S. A. Voloshin, Radial and elliptic flow at rhic: Further predictions, Phys. Lett. B503 (2001) 58–64

  15. [15]

    Collective flow and two-pion correlations from a relativistic hydrodynamic model with early chemical freeze out

    T. Hirano, K. Tsuda, Collective flow and two pion correlations from a relativistic hydrodynamic model with early chemical freeze out, Phys. Rev. C66 (2002) 054905. arXiv:nucl-th/0205043, doi:10.1103/PhysRevC.66.054905

  16. [16]

    Viscosity Information from Relativistic Nuclear Collisions: How Perfect is the Fluid Observed at RHIC?

    P. Romatschke, U. Romatschke, Viscosity In- formation from Relativistic Nuclear Collisions: How Perfect is the Fluid Observed at RHIC?, Phys.Rev.Lett. 99 (2007) 172301. arXiv:0706.1522, doi:10.1103/PhysRevLett.99.172301

  17. [17]

    Flow fluctuations and long-range correlations: elliptic flow and beyond

    M. Luzum, Flow fluctuations and long-range correlations: elliptic flow and beyond, J. Phys. G38 (2011) 124026. arXiv:1107.0592, doi:10.1088/0954-3899/38/12/124026

  18. [18]

    H. Song, S. A. Bass, U. Heinz, T. Hirano, C. Shen, 200 A GeV Au+Au collisions serve a nearly perfect quark-gluon liquid, Phys. Rev. Lett. 106 (2011) 192301, [Erratum: Phys. Rev. Lett.109,139904(2012)]. arXiv:1011.2783, doi:10.1103/PhysRevLett.106.192301,10.1103/PhysRevLett.109.139904

  19. [19]

    J. Qian, U. W. Heinz, J. Liu, Mode-coupling ef- fects in anisotropic flow in heavy-ion collisions, Phys. Rev. C93 (6) (2016) 064901. arXiv:1602.02813, doi:10.1103/PhysRevC.93.064901

  20. [20]

    Anisotropic flow in sqrt(s)=2.76 TeV Pb+Pb collisions at the LHC

    B. Schenke, S. Jeon, C. Gale, Anisotropic flow in√ s = 2 .76 TeV Pb+Pb collisions at the LHC, Phys.Lett. B702 (2011) 59–63. arXiv:1102.0575, doi:10.1016/j.physletb.2011.06.065

  21. [21]

    Magdy, X

    N. Magdy, X. Sun, Z. Ye, O. Evdokimov, R. Lacey, Investigation of the Elliptic Flow Fluctuations of the Identified Particles Using the a Multi-Phase Transport Model, Universe 6 (9) (2020) 146. arXiv:2009.02734, doi:10.3390/universe6090146

  22. [22]

    Magdy, Characterizing initial- and final-state ef- fects of relativistic nuclear collisions, Phys

    N. Magdy, Characterizing initial- and final-state ef- fects of relativistic nuclear collisions, Phys. Rev. C 107 (2) (2023) 024905. arXiv:2210.14091, doi:10.1103/PhysRevC.107.024905

  23. [23]

    Flow Study in Relativistic Nuclear Collisions by Fourier Expansion of Azimuthal Particle Distributions

    S. Voloshin, Y. Zhang, Flow study in relativistic nu- clear collisions by Fourier expansion of Azimuthal par- ticle distributions, Z. Phys. C 70 (1996) 665–672. arXiv:hep-ph/9407282, doi:10.1007/s002880050141

  24. [24]

    A. M. Poskanzer, S. A. Voloshin, Methods for analyzing anisotropic flow in relativistic nuclear collisions, Phys. Rev. C58 (1998) 1671–1678. arXiv:nucl-ex/9805001, doi:10.1103/PhysRevC.58.1671

  25. [25]

    Alver, et al., System size, energy, pseudorapid- ity, and centrality dependence of elliptic flow, Phys

    B. Alver, et al., System size, energy, pseudorapid- ity, and centrality dependence of elliptic flow, Phys. Rev. Lett. 98 (2007) 242302. arXiv:nucl-ex/0610037, doi:10.1103/PhysRevLett.98.242302

  26. [26]

    Adler, et al., Elliptic flow from two and four particle correlations in Au+Au collisions at √ SN N = 130-GeV, Phys

    C. Adler, et al., Elliptic flow from two and four particle correlations in Au+Au collisions at √ SN N = 130-GeV, Phys. Rev. C 66 (2002) 034904. doi:10.1103/PhysRevC.66.034904

  27. [27]

    Adams, et al., Azimuthal anisotropy at RHIC: The First and fourth harmonics, Phys

    J. Adams, et al., Azimuthal anisotropy at RHIC: The First and fourth harmonics, Phys. Rev. Lett. 92 (2004) 062301, [Erratum: Phys.Rev.Lett. 127, 069901 (2021)]. doi:10.1103/PhysRevLett.127.069901

  28. [28]

    Adare, et al., Measurement of two-particle corre- lations with respect to second- and third-order event planes in Au+Au collisions at √ sN N = 200 GeV, Phys

    A. Adare, et al., Measurement of two-particle corre- lations with respect to second- and third-order event planes in Au+Au collisions at √ sN N = 200 GeV, Phys. Rev. C 99 (5) (2019) 054903. arXiv:1803.01749, doi:10.1103/PhysRevC.99.054903

  29. [29]

    Aamodt, et al., Higher harmonic anisotropic flow measurements of charged particles in Pb-Pb collisions at √ sN N=2.76 TeV, Phys

    K. Aamodt, et al., Higher harmonic anisotropic flow measurements of charged particles in Pb-Pb collisions at √ sN N=2.76 TeV, Phys. Rev. Lett. 107 (2011) 032301. doi:10.1103/PhysRevLett.107.032301

  30. [30]

    Aaboud, et al., Measurement of the azimuthal anisotropy of charged particles produced in √sNN = 5.02 TeV Pb+Pb collisions with the ATLAS detector, Eur

    M. Aaboud, et al., Measurement of the azimuthal anisotropy of charged particles produced in √sNN = 5.02 TeV Pb+Pb collisions with the ATLAS detector, Eur. Phys. J. C 78 (12) (2018) 997. doi:10.1140/epjc/s10052-018-6468-7

  31. [31]

    Chatrchyan, et al., Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at √ sN N = 2 .76 TeV, Phys

    S. Chatrchyan, et al., Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at √ sN N = 2 .76 TeV, Phys. Rev. Lett. 109 (2012) 022301. doi:10.1103/PhysRevLett.109.022301

  32. [32]

    Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV

    S. Chatrchyan, et al., Measurement of the el- liptic anisotropy of charged particles produced in PbPb collisions at √ sN N=2.76 TeV, Phys. Rev. C 87 (1) (2013) 014902. arXiv:1204.1409, doi:10.1103/PhysRevC.87.014902

  33. [33]

    Magdy, Characterizing the initial- and final-state effects in isobaric collisions at energies available at the BNL Relativistic Heavy Ion Collider, Phys

    N. Magdy, Characterizing the initial- and final-state effects in isobaric collisions at energies available at the BNL Relativistic Heavy Ion Collider, Phys. Rev. C 109 (2) (2024) 024906. arXiv:2401.04083, doi:10.1103/PhysRevC.109.024906

  34. [34]

    Magdy, Beam-energy dependence of the azimuthal anisotropic flow from RHIC (2019)

    N. Magdy, Beam-energy dependence of the azimuthal anisotropic flow from RHIC (2019). arXiv:1909.09640

  35. [35]

    Azimuthal harmonics in small and large collision systems at RHIC top energies

    J. Adam, et al., Azimuthal Harmonics in Small and Large Collision Systems at RHIC Top Energies, Phys. Rev. Lett. 122 (17) (2019) 172301. arXiv:1901.08155, doi:10.1103/PhysRevLett.122.172301

  36. [36]

    Collision system and beam energy dependence of anisotropic flow fluctuations

    N. Magdy, Collision system and beam energy de- pendence of anisotropic flow fluctuations, Nucl. Phys. A982 (2019) 255–258. arXiv:1807.07638, doi:10.1016/j.nuclphysa.2018.09.027

  37. [37]

    Magdy, Beam Energy Dependence of the Linear and Mode-Coupled Flow Harmonics Using the a Multi- Phase Transport Model, Universe 9 (2) (2023) 107

    N. Magdy, Beam Energy Dependence of the Linear and Mode-Coupled Flow Harmonics Using the a Multi- Phase Transport Model, Universe 9 (2) (2023) 107. arXiv:2302.10373, doi:10.3390/universe9020107

  38. [38]

    Azimuthal anisotropy in Cu+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV

    L. Adamczyk, et al., Azimuthal anisotropy in Cu+Au collisions at √ sN N = 200 GeV, Phys. Rev. C98 (1) (2018) 014915. arXiv:1712.01332, doi:10.1103/PhysRevC.98.014915

  39. [39]

    Magdy, Viscous Damping of Anisotropic Flow in 7 .7 − 200 GeV Au+Au Collisions, J

    N. Magdy, Viscous Damping of Anisotropic Flow in 7 .7 − 200 GeV Au+Au Collisions, J. Phys. Conf. Ser. 779 (1) (2017) 012060. doi:10.1088/1742-6596/779/1/012060

  40. [40]

    Correlation Measurements Between Flow Harmonics in Au+Au Collisions at RHIC

    J. Adam, et al., Correlation Measurements Between Flow Harmonics in Au+Au Collisions at RHIC, Phys. Lett. B783 (2018) 459–465. arXiv:1803.03876, doi:10.1016/j.physletb.2018.05.076

  41. [41]

    Correlated event-by-event fluctuations of flow harmonics in Pb-Pb collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV

    J. Adam, et al., Correlated event-by-event fluctuations of flow harmonics in Pb-Pb col- lisions at √ sNN = 2 .76 TeV, Phys. Rev. Lett. 117 (2016) 182301. arXiv:1604.07663, 6 doi:10.1103/PhysRevLett.117.182301

  42. [42]

    Measurement of the correlation between flow harmonics of different order in lead-lead collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS detector

    G. Aad, et al., Measurement of the correlation be- tween flow harmonics of different order in lead-lead col- lisions at √ sN N=2.76 TeV with the ATLAS detector, Phys. Rev. C92 (3) (2015) 034903. arXiv:1504.01289, doi:10.1103/PhysRevC.92.034903

  43. [43]

    Z. Qiu, U. W. Heinz, Event-by-event shape and flow fluctuations of relativistic heavy-ion collision fireballs , Phys. Rev. C84 (2011) 024911. arXiv:1104.0650, doi:10.1103/PhysRevC.84.024911

  44. [44]

    Adare, et al., Measurements of Higher-Order Flow Harmonics in Au+Au Collisions at √sN N = 200 GeV, Phys

    A. Adare, et al., Measurements of Higher-Order Flow Harmonics in Au+Au Collisions at √sN N = 200 GeV, Phys. Rev. Lett. 107 (2011) 252301. arXiv:1105.3928, doi:10.1103/PhysRevLett.107.252301

  45. [45]

    Measurement of event-plane correlations in sqrt(s_NN)=2.76 TeV lead-lead collisions with the ATLAS detector

    G. Aad, et al., Measurement of event-plane correla- tions in √sN N = 2.76 TeV lead-lead collisions with the ATLAS detector, Phys. Rev. C90 (2) (2014) 024905. arXiv:1403.0489, doi:10.1103/PhysRevC.90.024905

  46. [46]

    The Importance of Correlations and Fluctuations on the Initial Source Eccentricity in High-Energy Nucleus-Nucleus Collisions

    B. Alver, et al., Importance of correlations and fluctuations on the initial source eccentricity in high-energy nucleus-nucleus collisions, Phys. Rev. C77 (2008) 014906. arXiv:0711.3724, doi:10.1103/PhysRevC.77.014906

  47. [47]

    Alver, et al., Non-flow correlations and elliptic flow fluctuations in gold-gold collisions at √ sN N = 200 GeV, Phys

    B. Alver, et al., Non-flow correlations and elliptic flow fluctuations in gold-gold collisions at √ sN N = 200 GeV, Phys. Rev. C81 (2010) 034915. arXiv:1002.0534, doi:10.1103/PhysRevC.81.034915

  48. [48]

    Effect of flow fluctuations and nonflow on elliptic flow methods

    J.-Y. Ollitrault, A. M. Poskanzer, S. A. Voloshin, Effec t of flow fluctuations and nonflow on elliptic flow meth- ods, Phys. Rev. C80 (2009) 014904. arXiv:0904.2315, doi:10.1103/PhysRevC.80.014904

  49. [49]

    Constraining models of initial conditions with elliptic and triangular flow data

    E. Retinskaya, M. Luzum, J.-Y. Ollitrault, Constrain- ing models of initial conditions with elliptic and trian- gular flow data, Phys. Rev. C 89 (1) (2014) 014902. arXiv:1311.5339, doi:10.1103/PhysRevC.89.014902

  50. [50]

    J. S. Moreland, J. E. Bernhard, S. A. Bass, Alter- native ansatz to wounded nucleon and binary colli- sion scaling in high-energy nuclear collisions, Phys. Rev. C 92 (1) (2015) 011901. arXiv:1412.4708, doi:10.1103/PhysRevC.92.011901

  51. [51]

    The Effect of Shear Viscosity on Spectra, Elliptic Flow, and HBT Radii

    D. Teaney, The Effects of viscosity on spec- tra, elliptic flow, and HBT radii, Phys.Rev. C68 (2003) 034913. arXiv:nucl-th/0301099, doi:10.1103/PhysRevC.68.034913

  52. [52]

    H. Song, S. A. Bass, U. Heinz, Elliptic flow in 200 A GeV Au+Au collisions and 2.76 A TeV Pb+Pb collisions: insights from viscous hy- drodynamics + hadron cascade hybrid model, Phys.Rev. C83 (2011) 054912. arXiv:1103.2380, doi:10.1103/PhysRevC.83.054912,10.1103/PhysRevC.87.019902

  53. [53]

    C. Shen, U. Heinz, P. Huovinen, H. Song, Ra- dial and elliptic flow in Pb+Pb collisions at the Large Hadron Collider from viscous hydrodynamic, Phys. Rev. C 84 (2011) 044903. arXiv:1105.3226, doi:10.1103/PhysRevC.84.044903

  54. [54]

    Giacalone, B

    G. Giacalone, B. Schenke, C. Shen, Observ- able signatures of initial state momentum anisotropies in nuclear collisions, Phys. Rev. Lett. 125 (19) (2020) 192301. arXiv:2006.15721, doi:10.1103/PhysRevLett.125.192301

  55. [55]

    Transverse momentum-flow correlations in relativistic heavy-ion collisions

    P. Bozek, Transverse-momentum–flow correla- tions in relativistic heavy-ion collisions, Phys. Rev. C 93 (4) (2016) 044908. arXiv:1601.04513, doi:10.1103/PhysRevC.93.044908

  56. [56]

    Schenke, C

    B. Schenke, C. Shen, D. Teaney, Transverse mo- mentum fluctuations and their correlation with elliptic flow in nuclear collision, Phys. Rev. C 102 (3) (2020) 034905. arXiv:2004.00690, doi:10.1103/PhysRevC.102.034905

  57. [57]

    Giacalone, F

    G. Giacalone, F. G. Gardim, J. Noronha-Hostler, J.- Y. Ollitrault, Correlation between mean transverse mo- mentum and anisotropic flow in heavy-ion collisions, Phys. Rev. C 103 (2) (2021) 024909. arXiv:2004.01765, doi:10.1103/PhysRevC.103.024909

  58. [58]

    S. H. Lim, J. L. Nagle, Exploring Origins for Correla- tions between Flow Harmonics and Transverse Momen- tum in Small Collision Systems (Unambiguous Ambi- guity) (3 2021). arXiv:2103.01348

  59. [59]

    Measurement of flow and transverse momentum corre- lations in Pb+Pb collisions at √ sNN = 5 .02 TeV and Xe+Xe collisions at √sNN = 5.44 TeV with the ATLAS detector (1 2021)

  60. [60]

    Transverse-momentum fluctuations in relativistic heavy-ion collisions from event-by-event viscous hydrodynamics

    P. Bozek, W. Broniowski, Transverse-momentum fluctuations in relativistic heavy-ion collisions from event-by-event viscous hydrodynamics, Phys. Rev. C 85 (2012) 044910. arXiv:1203.1810, doi:10.1103/PhysRevC.85.044910

  61. [61]

    Giacalone, Observing the deformation of nu- clei with relativistic nuclear collisions, Phys

    G. Giacalone, Observing the deformation of nu- clei with relativistic nuclear collisions, Phys. Rev. Lett. 124 (20) (2020) 202301. arXiv:1910.04673, doi:10.1103/PhysRevLett.124.202301

  62. [62]

    Giacalone, Constraining the quadrupole deforma- tion of atomic nuclei with relativistic nuclear collisions , Phys

    G. Giacalone, Constraining the quadrupole deforma- tion of atomic nuclei with relativistic nuclear collisions , Phys. Rev. C 102 (2) (2020) 024901. arXiv:2004.14463, doi:10.1103/PhysRevC.102.024901

  63. [63]

    Magdy, Impact of nuclear deformation on collec- tive flow observables in relativistic U+U collisions, Eur

    N. Magdy, Impact of nuclear deformation on collec- tive flow observables in relativistic U+U collisions, Eur. Phys. J. A 59 (3) (2023) 64. arXiv:2206.05332, doi:10.1140/epja/s10050-023-00982-0

  64. [64]

    arXiv:2401.06625

    Imaging Shapes of Atomic Nuclei in High-Energy Nu- clear Collisions (1 2024). arXiv:2401.06625

  65. [65]

    M. E. Beddo, et al., STAR: Conceptual design report for the Solenoidal Tracker at RHIC (6 1992)

  66. [66]

    The STAR Time Projection Chamber: A Unique Tool for Studying High Multiplicity Events at RHIC

    M. Anderson, et al., The Star time projection chamber: A Unique tool for studying high mul- tiplicity events at RHIC, Nucl. Instrum. Meth. A499 (2003) 659–678. arXiv:nucl-ex/0301015, doi:10.1016/S0168-9002(02)01964-2

  67. [67]

    Adamczyk, et al., Inclusive charged hadron el- liptic flow in Au + Au collisions at √ sN N = 7.7 - 39 GeV, Phys

    L. Adamczyk, et al., Inclusive charged hadron el- liptic flow in Au + Au collisions at √ sN N = 7.7 - 39 GeV, Phys. Rev. C 86 (2012) 054908. doi:10.1103/PhysRevC.86.054908

  68. [68]

    B. I. Abelev, et al., Identified particle pro- duction, azimuthal anisotropy, and interferome- try measurements in Au+Au collisions at √ SN N = 9.2- GeV, Phys. Rev. C 81 (2010) 024911. doi:10.1103/PhysRevC.81.024911

  69. [69]

    J. Jia, S. Mohapatra, Disentangling flow and non- flow correlations via Bayesian unfolding of the event-by-event distributions of harmonic coeffi- cients in ultrarelativistic heavy-ion collisions, Phys. Rev. C 88 (1) (2013) 014907. arXiv:1304.1471, doi:10.1103/PhysRevC.88.014907

  70. [70]

    J. Jia, M. Zhou, A. Trzupek, Revealing long-range multiparticle collectivity in small collision systems via subevent cumulants, Phys. Rev. C96 (3) (2017) 034906. arXiv:1701.03830, doi:10.1103/PhysRevC.96.034906

  71. [71]

    P. Huo, K. Gajdoˇ sov´ a, J. Jia, Y. Zhou, Im- portance of non-flow in mixed-harmonic multi- particle correlations in small collision systems, Phys. 7 Lett. B 777 (2018) 201–206. arXiv:1710.07567, doi:10.1016/j.physletb.2017.12.035

  72. [72]

    Non-flow effects in three-particle mixed-harmonic azimuthal correlations in small collision systems

    C. Zhang, J. Jia, J. Xu, Non-flow effects in three-particle mixed-harmonic azimuthal corre- lations in small collision systems, Phys. Lett. B792 (2019) 138–141. arXiv:1812.03536, doi:10.1016/j.physletb.2019.03.035

  73. [73]

    Magdy, O

    N. Magdy, O. Evdokimov, R. A. Lacey, A method to test the coupling strength of the linear and nonlinear contributions to higher-order flow harmonics via Event Shape Engineering, J. Phys. G 48 (2) (2020) 025101. arXiv:2002.04583, doi:10.1088/1361-6471/abcb59

  74. [74]

    Zhang, A

    C. Zhang, A. Behera, S. Bhatta, J. Jia, Non-flow effects in correlation between harmonic flow and transverse momentum in nuclear collisions (2 2021). arXiv:2102.05200

  75. [75]

    Magdy, Measuring differential flow angle fluctu- ations in relativistic nuclear collisions, Phys

    N. Magdy, Measuring differential flow angle fluctu- ations in relativistic nuclear collisions, Phys. Rev. C 106 (4) (2022) 044911. arXiv:2207.04530, doi:10.1103/PhysRevC.106.044911

  76. [76]

    Bozek, R

    P. Bozek, R. Samanta, Higher order cumulants of transverse momentum and harmonic flow in relativistic heavy ion collisions, Phys. Rev. C 104 (1) (2021) 014905. arXiv:2103.15338, doi:10.1103/PhysRevC.104.014905

  77. [78]

    B. B. Abelev, et al., Event-by-event mean pT fluctu- ations in pp and Pb-Pb collisions at the LHC, Eur. Phys. J. C 74 (10) (2014) 3077. arXiv:1407.5530, doi:10.1140/epjc/s10052-014-3077-y

  78. [79]

    Aad, et al., Measurement of flow harmon- ics correlations with mean transverse momentum in lead-lead and proton-lead collisions at √ sN N = 5.02 TeV with the ATLAS detector, Eur

    G. Aad, et al., Measurement of flow harmon- ics correlations with mean transverse momentum in lead-lead and proton-lead collisions at √ sN N = 5.02 TeV with the ATLAS detector, Eur. Phys. J. C 79 (12) (2019) 985. arXiv:1907.05176, doi:10.1140/epjc/s10052-019-7489-6

  79. [80]

    Bozek, H

    P. Bozek, H. Mehrabpour, Correlation coef- ficient between harmonic flow and transverse momentum in heavy-ion collisions, Phys. Rev. C 101 (6) (2020) 064902. arXiv:2002.08832, doi:10.1103/PhysRevC.101.064902

  80. [81]

    Multi-particle and charge-dependent azimuthal correlations in heavy-ion collisions at the Relativistic Heavy-Ion Collider

    B. Schenke, C. Shen, P. Tribedy, Multi-particle and charge-dependent azimuthal correlations in heavy-ion collisions at the Relativistic Heavy-Ion Collider, Phys. Rev. C 99 (4) (2019) 044908. arXiv:1901.04378, doi:10.1103/PhysRevC.99.044908

Showing first 80 references.