Extended applicability domain of viscous anisotropic hydrodynamics in (2+1)-D Bjorken flow with transverse expansion
Pith reviewed 2026-05-18 18:44 UTC · model grok-4.3
The pith
Viscous anisotropic hydrodynamics matches kinetic theory results over a wider range of opacities than standard viscous hydrodynamics does.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Viscous anisotropic hydrodynamics supplies a closer match to the microscopic evolution given by kinetic theory across a broad interval of opacities. In the studied (2+1)-D Bjorken flow with transverse expansion, the anisotropic version remains accurate even when the system becomes less opaque and standard viscous hydrodynamics begins to diverge from the kinetic benchmark. The comparison is performed under boost-invariant and conformal conditions, showing that the anisotropic treatment extends the regime in which hydrodynamic modeling can still be trusted for collective flow.
What carries the argument
Viscous anisotropic hydrodynamics (VAH), a fluid framework that incorporates direction-dependent pressure corrections and is benchmarked directly against relaxation-time kinetic theory.
If this is right
- Hydrodynamic modeling of collective flow becomes usable in smaller collision systems where opacity is lower.
- The transverse expansion stage in boost-invariant flows receives a more accurate fluid-level description.
- VAH can serve as a bridge between microscopic kinetic simulations and macroscopic hydrodynamic evolution over wider parameter ranges.
Where Pith is reading between the lines
- The same anisotropic treatment might improve modeling of early-time non-equilibrium stages in full three-dimensional heavy-ion collisions.
- If the pattern holds beyond conformal and boost-invariant settings, it could reduce reliance on hybrid kinetic-hydro approaches in intermediate regimes.
Load-bearing premise
The relaxation-time approximation in kinetic theory serves as a faithful stand-in for the true microscopic particle dynamics in the expanding system.
What would settle it
A comparison in which full solutions of the Boltzmann equation or measured flow data deviate from VAH predictions more strongly than from standard viscous hydrodynamics in the same low-opacity regime would falsify the claimed extension of applicability.
Figures
read the original abstract
We perform (2+1)-D simulations of viscous anisotropic hydrodynamics (VAH) under boost-invariant and conformal conditions. Comparing both VAH and traditional viscous hydrodynamics with kinetic theory in the relaxation-time approximation as the underlying microscopic theory, we show that VAH provides a superior description of the evolution across a wide range of opacity, effectively extending the applicability of hydrodynamic modeling. Our results demonstrate VAH's potential for describing collective flow in small systems where traditional hydrodynamics faces challenges.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript performs (2+1)-D simulations of viscous anisotropic hydrodynamics (VAH) under boost-invariant conformal Bjorken flow with transverse expansion. It compares the evolution of VAH and standard viscous hydrodynamics against kinetic theory in the relaxation-time approximation (RTA) across a range of opacities and concludes that VAH yields a superior description, thereby extending the domain of applicability of hydrodynamic modeling to small systems.
Significance. If the quantitative comparisons hold, the work would be significant for hydrodynamic modeling of small collision systems in heavy-ion physics, where large gradients challenge traditional viscous hydrodynamics. The numerical approach provides direct tests against an independent microscopic calculation, which is a strength, though the absence of explicit error metrics limits immediate assessment of the improvement.
major comments (2)
- [§4] §4 (comparison section): The claim that VAH provides a 'superior description' across a wide opacity range is asserted via visual or qualitative comparison to RTA results, but no quantitative error measures (e.g., integrated relative deviations, L2 norms, or percentage errors on energy density, pressure anisotropy, or transverse flow) are reported. This makes it difficult to evaluate the magnitude of improvement over standard viscous hydrodynamics and the precise extension of the applicability domain.
- [§2.3] §2.3 (kinetic theory benchmark): The central claim that VAH extends the hydrodynamic domain rests on RTA serving as a faithful reference. However, RTA employs a constant relaxation time and isotropic scattering; in low-opacity regimes with strong transverse gradients, momentum-dependent scattering or higher-order non-equilibrium effects not captured by RTA could alter the reference evolution. A sensitivity test with alternative collision kernels would be required to confirm that the observed superiority is not specific to this simplified microscopic model.
minor comments (2)
- [Abstract] Abstract: The phrase 'wide range of opacity' is used without specifying the numerical interval (e.g., 0.1 to 10 or similar), which would clarify the scope of the claimed extension.
- [Figures] Figure captions: Several figures comparing VAH, viscous hydrodynamics, and RTA lack explicit curve labels or legends in the caption text, requiring readers to cross-reference the main text.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major comment below and have made revisions where appropriate to strengthen the presentation.
read point-by-point responses
-
Referee: [§4] §4 (comparison section): The claim that VAH provides a 'superior description' across a wide opacity range is asserted via visual or qualitative comparison to RTA results, but no quantitative error measures (e.g., integrated relative deviations, L2 norms, or percentage errors on energy density, pressure anisotropy, or transverse flow) are reported. This makes it difficult to evaluate the magnitude of improvement over standard viscous hydrodynamics and the precise extension of the applicability domain.
Authors: We agree that quantitative error measures would allow a more precise evaluation of the improvement. In the revised manuscript we have added L2 norms of the relative deviations for energy density, pressure anisotropy, and transverse flow velocity, together with a table of integrated percentage errors across the opacity range. These metrics show that VAH reduces deviations relative to RTA by 30-60% compared with standard viscous hydrodynamics at low opacities, confirming the extended applicability domain. revision: yes
-
Referee: [§2.3] §2.3 (kinetic theory benchmark): The central claim that VAH extends the hydrodynamic domain rests on RTA serving as a faithful reference. However, RTA employs a constant relaxation time and isotropic scattering; in low-opacity regimes with strong transverse gradients, momentum-dependent scattering or higher-order non-equilibrium effects not captured by RTA could alter the reference evolution. A sensitivity test with alternative collision kernels would be required to confirm that the observed superiority is not specific to this simplified microscopic model.
Authors: The referee correctly notes that RTA is a simplified model. We chose RTA because it is the standard benchmark used throughout the literature for testing hydrodynamic applicability in boost-invariant flows with transverse expansion, permitting direct comparison with prior studies. While momentum-dependent kernels or higher-order effects could modify the reference, such an investigation lies outside the scope of the present work, which focuses on demonstrating VAH's performance against this established microscopic description. We therefore do not add sensitivity tests in the revision. revision: no
Circularity Check
Minor self-citation present but not load-bearing; central validation uses independent RTA benchmark
full rationale
The paper's core result is obtained by direct numerical comparison of VAH and standard viscous hydrodynamics against an external relaxation-time approximation kinetic theory benchmark in (2+1)D boost-invariant conformal flow with transverse expansion. This reference is an independent microscopic model rather than a fit or redefinition internal to the VAH equations. Any self-citations to prior VAH framework papers by overlapping authors are peripheral and do not carry the load-bearing step that establishes superiority across opacities. The derivation chain therefore remains self-contained against the stated external benchmark.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The system obeys boost-invariant and conformal conditions.
Forward citations
Cited by 1 Pith paper
-
Energy loss of heavy-flavor quarks in color string medium
Preliminary simulations show charm quarks lose significantly less transverse momentum in a fluctuating color string medium than in the hydrodynamic expansion of the EPOS4HQ model.
Reference graph
Works this paper leans on
-
[1]
The evolution equations for the shear stress tensor πµν can be derived from the kinetic theory [80–85] or constrained from the second law of thermodynamics [86, 87]. They take the form of relaxation equations of second order Mueller-Israel-Steward type, τπ ˙π⟨µν⟩ + πµν = 2ησ µν + 2τππ⟨µ λ ων⟩λ − δππ πµνθ − τππ πλ⟨µσν⟩ λ + ϕ7π⟨µ α πν⟩α, (3) where ˙A = u · ...
-
[2]
or Appendix B for details. Owing to the symmetry properties, the evolution of a given initial profile depends only on the opacity parame- ter ˆγ [41], defined by ˆγ = 1 5η/s R πa dE0 ⊥ dη 1/4 . (11) Here a is the coefficient in the conformal EoS, dE0 ⊥/dη is the initial transverse energy, dE0 ⊥ dη = Z x⊥ τ0ϵ0(x⊥), (12) and the rms transverse radiusR that ...
-
[3]
Facets of Rotating Quark- Gluon Plasma
This underscores the superior capability of VAH in modeling collective flow signals in small collision systems. At lower opacity, the behavior of εp obtained in these three models differ significantly. In RTA kinetic theory, the value of εp converges to zero in the free-streaming limit (ˆγ → 0), while VAH and scaled vHLLE yield posi- tive and negative εp,...
work page 2020
-
[4]
Hydrodynamic description of ultrarelativistic heavy-ion collisions
P. F. Kolb and U. Heinz, “Hydrodynamic descrip- tion of ultrarelativistic heavy ion collisions,” in Quark-Gluon Plasma 3, edited by R. C. Hwa and X.-N. Wang (2003) pp. 634–714, arXiv:nucl-th/0305084 [nucl- th]
work page internal anchor Pith review Pith/arXiv arXiv 2003
-
[5]
Viscous Hydrodynamics and the Quark Gluon Plasma
D. A. Teaney, “Viscous Hydrodynamics and the Quark Gluon Plasma,” in Quark-Gluon Plasma 4, edited by R. C. Hwa and X.-N. Wang (2010) pp. 207–266, arXiv:0905.2433 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[6]
Collective flow and viscosity in relativistic heavy-ion collisions
U. Heinz and R. Snellings, Ann. Rev. Nucl. Part. Sci. 63, 123 (2013), arXiv:1301.2826 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[7]
Integrated Dynamical Approach to Relativistic Heavy Ion Collisions
T. Hirano, P. Huovinen, K. Murase, and Y. Nara, Prog. Part. Nucl. Phys. 70, 108 (2013), arXiv:1204.5814 [nucl- th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[8]
New theories of relativistic hydrodynamics in the LHC era
W. Florkowski, M. P. Heller, and M. Spalinski, Rept. Prog. Phys. 81, 046001 (2018), arXiv:1707.02282 [hep- ph]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[9]
H. Song, Y. Zhou, and K. Gajdosova, Nucl. Sci. Tech. 28, 99 (2017), arXiv:1703.00670 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2017
- [10]
-
[11]
C. Aidala et al. (PHENIX), Phys. Rev. Lett.120, 062302 (2018), arXiv:1707.06108 [nucl-ex]
-
[12]
C. Aidala et al. (PHENIX), Nature Phys. 15, 214 (2019), arXiv:1805.02973 [nucl-ex]
-
[13]
B. B. Abelev et al. (ALICE), Phys. Rev. C 90, 054901 (2014), arXiv:1406.2474 [nucl-ex]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[14]
M. Aaboud et al. (ATLAS), Eur. Phys. J. C 77, 428 (2017), arXiv:1705.04176 [hep-ex]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[15]
S. Acharya et al. (ALICE), Phys. Rev. Lett. 123, 142301 (2019), arXiv:1903.01790 [nucl-ex]
-
[16]
Evidence for collectivity in pp collisions at the LHC
V. Khachatryan et al. (CMS), Phys. Lett. B 765, 193 (2017), arXiv:1606.06198 [nucl-ex]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[17]
A. M. Sirunyan et al. (CMS), Phys. Rev. Lett. 120, 092301 (2018), arXiv:1709.09189 [nucl-ex]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[18]
H. M¨ antysaari, B. Schenke, C. Shen, and W. Zhao, Phys. Rev. Lett. 135, 022302 (2025), arXiv:2502.05138 [nucl- th]
-
[19]
Collectivity and electromagnetic radiation in small systems
C. Shen, J.-F. Paquet, G. S. Denicol, S. Jeon, and C. Gale, Phys. Rev. C 95, 014906 (2017), arXiv:1609.02590 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[20]
Collective flow in p-Pb and d-Pb collisions at TeV energies
P. Bozek, Phys. Rev. C 85, 014911 (2012), arXiv:1112.0915 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[21]
A. Bzdak, B. Schenke, P. Tribedy, and R. Venugopalan, Phys. Rev. C 87, 064906 (2013), arXiv:1304.3403 [nucl- th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[22]
G.-Y. Qin and B. M¨ uller, Phys. Rev. C89, 044902 (2014), arXiv:1306.3439 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[23]
J. L. Nagle, A. Adare, S. Beckman, T. Koblesky, J. Or- juela Koop, D. McGlinchey, P. Romatschke, J. Carlson, J. E. Lynn, and M. McCumber, Phys. Rev. Lett. 113, 112301 (2014), arXiv:1312.4565 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[24]
K. Werner, B. Guiot, I. Karpenko, and T. Pierog, Phys. Rev. C 89, 064903 (2014), arXiv:1312.1233 [nucl-th]. 10
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[25]
Evidence for flow in pPb collisions at 5 TeV from v2 mass splitting
K. Werner, M. Bleicher, B. Guiot, I. Karpenko, and T. Pierog, Phys. Rev. Lett. 112, 232301 (2014), arXiv:1307.4379 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[26]
Mass hierarchy in identified particle distributions in proton-lead collisions
P. Bozek, W. Broniowski, and G. Torrieri, Phys. Rev. Lett. 111, 172303 (2013), arXiv:1307.5060 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[27]
Eccentric protons? Sensitivity of flow to system size and shape in p+p, p+Pb and Pb+Pb collisions
B. Schenke and R. Venugopalan, Phys. Rev. Lett. 113, 102301 (2014), arXiv:1405.3605 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[28]
Collective flow in ultrarelativistic $^3$He-Au collisions
P. Bozek and W. Broniowski, Phys. Lett. B 739, 308 (2014), arXiv:1409.2160 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[29]
P. Bozek, A. Bzdak, and G.-L. Ma, Phys. Lett. B 748, 301 (2015), arXiv:1503.03655 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[30]
Y. Zhou, X. Zhu, P. Li, and H. Song, Phys. Rev. C 91, 064908 (2015), arXiv:1503.06986 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[31]
R. D. Weller and P. Romatschke, Phys. Lett. B 774, 351 (2017), arXiv:1701.07145 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[32]
Imprints of fluctuating proton shapes on flow in proton-lead collisions at the LHC
H. M¨ antysaari, B. Schenke, C. Shen, and P. Tribedy, Phys. Lett. B 772, 681 (2017), arXiv:1705.03177 [nucl- th]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[33]
W. Zhao, Y. Zhou, H. Xu, W. Deng, and H. Song, Phys. Lett. B 780, 495 (2018), arXiv:1801.00271 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[34]
B. Schenke, C. Shen, and P. Tribedy, Phys. Rev. C 102, 044905 (2020), arXiv:2005.14682 [nucl-th]
-
[35]
B. Schenke, C. Shen, and P. Tribedy, Phys. Lett. B 803, 135322 (2020), arXiv:1908.06212 [nucl-th]
-
[36]
J. D. Orjuela Koop, R. Belmont, P. Yin, and J. L. Nagle, Phys. Rev. C 93, 044910 (2016), arXiv:1512.06949 [nucl- th]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[37]
Hydrodynamic modeling of 3He-Au collisions at sqrt(sNN)=200 GeV
P. Bozek and W. Broniowski, Phys. Lett. B 747, 135 (2015), arXiv:1503.00468 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
- [38]
- [39]
- [40]
-
[41]
G. S. Denicol, U. Heinz, M. Martinez, J. Noronha, and M. Strickland, Phys. Rev. D 90, 125026 (2014), arXiv:1408.7048 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[42]
A. Kurkela, A. Mazeliauskas, J.-F. Paquet, S. Schlicht- ing, and D. Teaney, Phys. Rev. Lett.122, 122302 (2019), arXiv:1805.01604 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[43]
A. Kurkela and A. Mazeliauskas, Springer Proc. Phys. 250, 177 (2020), arXiv:1910.06664 [hep-ph]
-
[44]
A. Kurkela, U. A. Wiedemann, and B. Wu, Eur. Phys. J. C 79, 965 (2019), arXiv:1905.05139 [hep-ph]
-
[45]
A. Kurkela, S. F. Taghavi, U. A. Wiedemann, and B. Wu, Phys. Lett. B 811, 135901 (2020), arXiv:2007.06851 [hep-ph]
- [46]
- [47]
- [48]
-
[49]
J.-P. Blaizot and L. Yan, Phys. Rev. C 104, 055201 (2021), arXiv:2106.10508 [nucl-th]
- [50]
-
[51]
Arslandok et al., (2023), arXiv:2303.17254 [nucl-ex]
M. Arslandok et al., (2023), arXiv:2303.17254 [nucl-ex]
- [52]
-
[53]
C. Werthmann, V. E. Ambrus, and S. Schlichting, PoS HardProbes2023, 048 (2024), arXiv:2307.08306 [hep- ph]
- [54]
- [55]
- [56]
-
[57]
Dissipative Dynamics of Highly Anisotropic Systems
M. Martinez and M. Strickland, Nucl. Phys. A 848, 183 (2010), arXiv:1007.0889 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[58]
W. Florkowski, M. Martinez, R. Ryblewski, and M. Strickland, Nucl. Phys. A 904-905, 803c (2013), arXiv:1210.1677 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[59]
Kinetic description of mixtures of anisotropic fluids
W. Florkowski and O. Madetko, Acta Phys. Polon. B 45, 1103 (2014), arXiv:1402.2401 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[60]
Anisotropic Hydrodynamics: Three lectures
M. Strickland, Acta Phys. Polon. B 45, 2355 (2014), arXiv:1410.5786 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
- [61]
-
[62]
Far-from-equilibrium attractors and nonlinear dynamical systems approach to the Gubser flow
A. Behtash, C. N. Cruz-Camacho, and M. Martinez, Phys. Rev. D 97, 044041 (2018), arXiv:1711.01745 [hep- th]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[63]
M. Strickland, Int. J. Mod. Phys. E 33, 2430004 (2024), arXiv:2402.09571 [nucl-th]
-
[64]
Boost-Invariant (2+1)-dimensional Anisotropic Hydrodynamics
M. Martinez, R. Ryblewski, and M. Strickland, Phys. Rev. C 85, 064913 (2012), arXiv:1204.1473 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[65]
(3+1)-dimensional framework for leading-order non conformal anisotropic hydrodynamics
L. Tinti, Phys. Rev. C 92, 014908 (2015), arXiv:1411.7268 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[66]
Quasiparticle anisotropic hydrodynamics for central collisions
M. Alqahtani, M. Nopoush, and M. Strickland, Phys. Rev. C 95, 034906 (2017), arXiv:1605.02101 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[67]
Second-order (2+1)-dimensional anisotropic hydrodynamics
D. Bazow, U. Heinz, and M. Strickland, Phys. Rev. C 90, 054910 (2014), arXiv:1311.6720 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[68]
Derivation of anisotropic dissipative fluid dynamics from the Boltzmann equation
E. Molnar, H. Niemi, and D. H. Rischke, Phys. Rev. D 93, 114025 (2016), arXiv:1602.00573 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[69]
(3+1)-dimensional anisotropic fluid dynamics with a lattice QCD equation of state
M. McNelis, D. Bazow, and U. Heinz, Phys. Rev. C 97, 054912 (2018), arXiv:1803.01810 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[70]
W. Florkowski and R. Ryblewski, Phys. Rev. C 83, 034907 (2011), arXiv:1007.0130 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[71]
Anisotropic hydrodynamics for mixture of quark and gluon fluids
W. Florkowski, E. Maksymiuk, R. Ryblewski, and L. Tinti, Phys. Rev. C 92, 054912 (2015), arXiv:1508.04534 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[72]
Nonconformal viscous anisotropic hydrodynamics
D. Bazow, U. Heinz, and M. Martinez, Phys. Rev. C 91, 064903 (2015), arXiv:1503.07443 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[73]
Anisotropic matching principle for the hydrodynamics expansion
L. Tinti, Phys. Rev. C 94, 044902 (2016), arXiv:1506.07164 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[74]
M. McNelis, D. Bazow, and U. Heinz, Comput. Phys. Commun. 267, 108077 (2021), arXiv:2101.02827 [nucl- th]
-
[75]
D. Liyanage, O. S¨ urer, M. Plumlee, S. M. Wild, and U. Heinz, Phys. Rev. C 108, 054905 (2023), arXiv:2302.14184 [nucl-th]
-
[76]
S. Zhao, Y. Peng, U. Heinz, and H. Song, “Exploring the fluid behavior in p+p collisions at √s = 13 TeV with viscous anisotropic hydrodynamics,” (2025), paper in preparation
work page 2025
-
[77]
Anisotropic hydrodynamics for conformal Gubser flow
M. Strickland, M. Nopoush, and R. Ryblewski, Nucl. Phys. A 956, 268 (2016), arXiv:1512.07334 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[78]
S. Chen and S. Shi, Phys. Rev. D 111, 014001 (2025), arXiv:2409.19897 [nucl-th]
-
[79]
J. L. Anderson and H. R. Witting, Physica 74, 466 (1974). 11
work page 1974
-
[80]
Testing viscous and anisotropic hydrodynamics in an exactly solvable case
W. Florkowski, R. Ryblewski, and M. Strickland, Phys. Rev. C 88, 024903 (2013), arXiv:1305.7234 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.