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arxiv: 2603.29325 · v2 · submitted 2026-03-31 · ✦ hep-ph · nucl-th

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· Lean Theorem

Baryonic vortices in rotating nuclear matter

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Pith reviewed 2026-05-13 23:58 UTC · model grok-4.3

classification ✦ hep-ph nucl-th
keywords baryonic vorticesrotating nuclear matterchiral perturbation theoryglobal vortexlocal vortextopological chargecausality regularizationdense QCD
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The pith

Causality bound in a rotating frame turns divergent global baryonic vortices into finite-energy excitations.

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

The paper establishes that baryonic vortices in rotating nuclear matter, modeled by chiral perturbation theory, exist in two forms carrying topological baryon charge from the third homotopy group of the three-sphere. Local vortices show charged-pion phase winding on the boundary and neutral-pion variation inside the core, while global vortices reverse this with neutral-pion condensate and winding plus internal charged-pion variation. Although global vortices normally suffer logarithmic energy divergence in infinite space, the finite radial size enforced by causality in the rotating frame cuts off the divergence and renders them stable. This leads to an energetic competition between the two vortex types controlled by rotation rate, system size, and baryon chemical potential, implying that global vortices can contribute to the topological structure of dense rotating QCD matter.

Core claim

In chiral perturbation theory applied to rotating nuclear matter, baryonic vortices are topological excitations classified by the third homotopy group of the three-sphere. Local vortices are built from charged-pion condensates with phase winding on the boundary and neutral-pion variation along the axis inside the core. Global vortices are instead formed by neutral-pion condensate and phase winding, with charged pions varying inside. The finite-size constraint imposed by causality in the rotating frame physically regularizes the usual logarithmic energy divergence of global vortices, making them viable finite-energy states that compete with local vortices as functions of rotation, system size

What carries the argument

The causality bound in the rotating frame, which imposes a finite radial cutoff that regularizes the logarithmic energy divergence of global vortices.

If this is right

  • Global vortices become energetically competitive with local vortices for ranges of rotation rate, system size, and baryon chemical potential.
  • The topological structure of rotating dense nuclear matter includes both local and global vortex configurations carrying baryon number.
  • Global vortices provide a previously overlooked channel for topological excitations in finite rotating systems.
  • The regularization allows global vortices to participate in the phase structure of dense QCD matter under rotation.

Where Pith is reading between the lines

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

  • In neutron-star interiors, global vortices could influence angular-momentum transport or glitch dynamics beyond what local vortices alone predict.
  • The same causality regularization may apply to other global defects in effective theories of dense matter, altering their stability in finite rotating volumes.
  • Simulations of rotating nuclear matter that incorporate the light-speed bound could reveal mixed vortex lattices containing both types.

Load-bearing premise

Chiral perturbation theory remains valid at the densities and rotation rates of interest, and the causality limit supplies a physical cutoff without requiring additional dynamical mechanisms.

What would settle it

A direct computation or simulation showing that the energy per unit length of the global vortex configuration continues to diverge logarithmically with system size even after the rotating-frame causality bound is imposed.

read the original abstract

We investigate baryonic vortices as topological excitations in rotating nuclear matter within the framework of chiral perturbation theory. We identify two distinct configurations: local and global vortices, both carrying the baryon number as the topological charge associated with the third homotopy group $\pi_3(S^3)$. For the local vortex, similar to the vortex Skyrmion in a finite isospin chemical potential, charged pions form the condensate on the boundary and have a phase winding, while the neutral pion varies along the rotation axis inside the vortex core. On the other hand, a global vortex is formed by the condensate and phase winding of the neutral pion, while the charged pions vary on the inside along the rotation axis. Crucially, although global vortices are usually discarded in infinite systems due to logarithmic divergence in energy, we demonstrate that the finite-size constraint dictated by causality in a rotating frame regularizes the divergence physically, rendering the global vortex a viable excitation. We reveal an energetic competition between global and local vortex states, under the tunable parameters of rotation, system size, and baryon chemical potential. Our results suggest that the previously overlooked global vortex can play a significant role in the topological structure of rotating dense QCD matter.

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

2 major / 2 minor

Summary. The manuscript investigates baryonic vortices as topological excitations in rotating nuclear matter within chiral perturbation theory. It identifies two configurations—local vortices with charged-pion condensate and phase winding on the boundary, and global vortices with neutral-pion condensate and phase winding—both carrying baryon number via the topological charge associated with π₃(S³). The central claim is that the finite-size constraint imposed by causality in the rotating frame (R < 1/ω) supplies a physical infrared cutoff that regularizes the usual logarithmic energy divergence of global vortices, rendering them viable; the work then compares the energies of the two vortex types as functions of rotation rate, system size, and baryon chemical potential.

Significance. If the regularization argument is made rigorous, the result would be significant for the topological structure of dense, rotating QCD matter, with potential relevance to neutron-star interiors. The use of standard homotopy classification and the effective-theory framework is a strength, as is the identification of an energetic competition between previously overlooked global vortices and local ones under tunable parameters.

major comments (2)
  1. [§3] §3 (global vortex construction): The claim that the causality bound R < 1/ω regularizes the logarithmic divergence relies on the standard ChPT energy functional remaining unmodified at large distances. The manuscript should provide an explicit integral evaluation (e.g., the neutral-pion kinetic term ∫ (∇θ)² r dr up to R = 1/ω) demonstrating convergence, and confirm that no frame-dependent corrections to the pion kinetic term or asymptotic profile arise in the rotating metric.
  2. [§4.1] §4.1 (energy comparison): The energetic competition between global and local vortices is presented as a function of rotation, size, and μ_B, but the manuscript does not show how the cutoff radius enters the local-vortex energy functional or whether the same causality bound applies uniformly; this affects the robustness of the phase diagram.
minor comments (2)
  1. [Abstract] The abstract refers to 'tunable parameters' without specifying their ranges; these should be stated explicitly when the energy functionals are introduced.
  2. [Introduction] Notation for the rotating-frame causality bound (R < 1/ω) should be defined at first use with a brief derivation or reference to the underlying metric.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address the major comments point by point below and have revised the manuscript accordingly to strengthen the presentation.

read point-by-point responses
  1. Referee: [§3] §3 (global vortex construction): The claim that the causality bound R < 1/ω regularizes the logarithmic divergence relies on the standard ChPT energy functional remaining unmodified at large distances. The manuscript should provide an explicit integral evaluation (e.g., the neutral-pion kinetic term ∫ (∇θ)² r dr up to R = 1/ω) demonstrating convergence, and confirm that no frame-dependent corrections to the pion kinetic term or asymptotic profile arise in the rotating metric.

    Authors: We agree that an explicit calculation clarifies the regularization. In the revised manuscript we have added an explicit evaluation of the neutral-pion kinetic term ∫ (∇θ)² r dr dφ dz integrated from the core radius ξ to the causality cutoff R = 1/ω. The integral yields a finite result proportional to log(1/(ω ξ)), which remains well-defined for any nonzero rotation rate. Within the leading-order chiral Lagrangian employed, frame-dependent corrections to the metric enter only at higher orders in the derivative expansion and do not modify the leading logarithmic infrared behavior or the asymptotic profile of the neutral pion. revision: yes

  2. Referee: [§4.1] §4.1 (energy comparison): The energetic competition between global and local vortices is presented as a function of rotation, size, and μ_B, but the manuscript does not show how the cutoff radius enters the local-vortex energy functional or whether the same causality bound applies uniformly; this affects the robustness of the phase diagram.

    Authors: We thank the referee for this observation. The same causality bound R < 1/ω is imposed uniformly on the system size for both configurations. For the local vortex the energy is already finite in infinite volume because the charged-pion condensate is exponentially localized; the additional integration up to R introduces only exponentially small corrections. In the revised §4.1 we have added explicit expressions for both energies as functions of R (with R = 1/ω) and confirmed that the relative ordering and the phase boundaries in the (ω, R, μ_B) space remain robust under this uniform cutoff. revision: yes

Circularity Check

0 steps flagged

Derivation chain is self-contained with no circular reductions

full rationale

The paper builds its analysis on the standard chiral perturbation theory Lagrangian and the topological classification of defects via the homotopy group π₃(S³), both of which are external to the present work. The central physical argument—that a causality bound in the rotating frame supplies a finite infrared cutoff for the global vortex energy—is introduced as an independent physical constraint on system size rather than a mathematical redefinition or fit to the vortex energy itself. No load-bearing step equates a derived quantity to an input parameter by construction, and self-citations to prior vortex literature serve only as background rather than as the sole justification for the regularization claim. The reported energetic competition between local and global vortices follows directly from minimizing the unmodified effective energy functional subject to the external cutoff.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on the applicability of chiral perturbation theory at the densities and rotations considered, plus standard topological classification via homotopy groups.

axioms (2)
  • domain assumption Chiral perturbation theory is valid for describing pion condensates in rotating nuclear matter at the relevant chemical potentials
    Framework invoked throughout the abstract for both vortex types
  • standard math The third homotopy group π3(S3) classifies the baryon number of the vortices
    Stated as the topological charge for both local and global configurations

pith-pipeline@v0.9.0 · 5509 in / 1232 out tokens · 41788 ms · 2026-05-13T23:58:02.310225+00:00 · methodology

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Reference graph

Works this paper leans on

55 extracted references · 55 canonical work pages · 4 internal anchors

  1. [1]

    H.-L. Chen, K. Fukushima, X.-G. Huang and K. Mameda,Analogy between rotation and density for Dirac fermions in a magnetic field,Phys. Rev. D93(2016) 104052 [1512.08974]

  2. [2]

    Jiang and J

    Y. Jiang and J. Liao,Pairing Phase Transitions of Matter under Rotation,Phys. Rev. Lett. 117(2016) 192302 [1606.03808]. – 13 –

  3. [3]

    Chernodub and S

    M.N. Chernodub and S. Gongyo,Interacting fermions in rotation: chiral symmetry restoration, moment of inertia and thermodynamics,JHEP01(2017) 136 [1611.02598]

  4. [4]

    Y. Chen, D. Li and M. Huang,Inhomogeneous chiral condensation under rotation in the holographic QCD,Phys. Rev. D106(2022) 106002 [2208.05668]

  5. [5]

    Chen, Z.-B

    H.-L. Chen, Z.-B. Zhu and X.-G. Huang,Quark-meson model under rotation: A functional renormalization group study,Phys. Rev. D108(2023) 054006 [2306.08362]

  6. [6]

    Fujimoto, K

    Y. Fujimoto, K. Fukushima and Y. Hidaka,Deconfining Phase Boundary of Rapidly Rotating Hot and Dense Matter and Analysis of Moment of Inertia,Phys. Lett. B816(2021) 136184 [2101.09173]

  7. [7]

    Chernodub,Inhomogeneous confining-deconfining phases in rotating plasmas,Phys

    M.N. Chernodub,Inhomogeneous confining-deconfining phases in rotating plasmas,Phys. Rev. D103(2021) 054027 [2012.04924]

  8. [8]

    Braga, L.F

    N.R.F. Braga, L.F. Faulhaber and O.C. Junqueira,Confinement-deconfinement temperature for a rotating quark-gluon plasma,Phys. Rev. D105(2022) 106003 [2201.05581]

  9. [9]

    X. Chen, L. Zhang, D. Li, D. Hou and M. Huang,Gluodynamics and deconfinement phase transition under rotation from holography,JHEP07(2021) 132 [2010.14478]

  10. [10]

    Huang, K

    X.-G. Huang, K. Nishimura and N. Yamamoto,Anomalous effects of dense matter under rotation,JHEP02(2018) 069 [1711.02190]

  11. [11]

    Nishimura and N

    K. Nishimura and N. Yamamoto,Topological term, QCD anomaly, and theη ′ chiral soliton lattice in rotating baryonic matter,JHEP07(2020) 196 [2003.13945]

  12. [12]

    M. Eto, K. Nishimura and M. Nitta,Phases of rotating baryonic matter: non-Abelian chiral soliton lattices, antiferro-isospin chains, and ferri/ferromagnetic magnetization,JHEP08 (2022) 305 [2112.01381]

  13. [13]

    M. Eto, K. Nishimura and M. Nitta,Domain-wall Skyrmion phase in a rapidly rotating QCD matter,JHEP03(2024) 019 [2310.17511]

  14. [14]

    M. Eto, K. Nishimura and M. Nitta,Non-Abelian chiral soliton lattice in rotating QCD matter: Nambu-Goldstone and excited modes,JHEP03(2024) 035 [2312.10927]

  15. [15]

    Witten,Global Aspects of Current Algebra,Nucl

    E. Witten,Global Aspects of Current Algebra,Nucl. Phys. B223(1983) 422

  16. [16]

    Evans, N

    G.W. Evans, N. Yamamoto and D.-L. Yang,Vorticity-induced effects from Wess-Zumino-Witten terms,2510.25459

  17. [17]

    Qiu and M

    Z. Qiu and M. Nitta,Baryonic vortex phase and magnetic field generation in QCD with isospin and baryon chemical potentials,JHEP06(2024) 139 [2403.07433]

  18. [18]

    Hamada, M

    Y. Hamada, M. Nitta and Z. Qiu,Baryons as linked vortices in QCD matter with isospin asymmetry,JHEP02(2026) 200 [2509.20844]

  19. [19]

    Hamada, M

    Y. Hamada, M. Nitta and Z. Qiu,QCD phase diagram in a magnetic field with baryon and isospin chemical potentials,2602.11762

  20. [20]

    Fukushima, K

    K. Fukushima, K. Hattori and K. Mameda,Preponderant Orbital Polarization in Relativistic Magnetovortical Matter, 9, 2024

  21. [21]

    Ebihara, K

    S. Ebihara, K. Fukushima and K. Mameda,Boundary effects and gapped dispersion in rotating fermionic matter,Phys. Lett. B764(2017) 94 [1608.00336]

  22. [22]

    Zhang, T

    X. Zhang, T. Huang and R.H. Brandenberger,Pion and eta strings,Phys. Rev. D58(1998) 027702 [hep-ph/9711452]. – 14 –

  23. [23]

    Berera, R

    A. Berera, R. Brandenberger, J. Mabillard and R.O. Ramos,Stability of the pion string in a thermal and dense medium,Phys. Rev. D94(2016) 065043 [1606.04113]

  24. [24]

    Abrikosov,On the Magnetic properties of superconductors of the second group,Sov

    A.A. Abrikosov,On the Magnetic properties of superconductors of the second group,Sov. Phys. JETP5(1957) 1174

  25. [25]

    Nielsen and P

    H.B. Nielsen and P. Olesen,Vortex Line Models for Dual Strings,Nucl. Phys. B61(1973) 45

  26. [26]

    Adhikari, T.D

    P. Adhikari, T.D. Cohen and J. Sakowitz,Finite Isospin Chiral Perturbation Theory in a Magnetic Field,Phys. Rev. C91(2015) 045202 [1501.02737]

  27. [27]

    Adhikari,Magnetic Vortex Lattices in Finite Isospin Chiral Perturbation Theory,Phys

    P. Adhikari,Magnetic Vortex Lattices in Finite Isospin Chiral Perturbation Theory,Phys. Lett. B790(2019) 211 [1810.03663]

  28. [28]

    Adhikari, E

    P. Adhikari, E. Leeser and J. Markowski,Phonon modes of magnetic vortex lattices in finite isospin chiral perturbation theory,Mod. Phys. Lett. A38(2023) 2350078 [2205.13369]

  29. [29]

    Grønli and T

    M.S. Grønli and T. Brauner,Competition of chiral soliton lattice and Abrikosov vortex lattice in QCD with isospin chemical potential,Eur. Phys. J. C82(2022) 354 [2201.07065]

  30. [30]

    Canfora, S

    F. Canfora, S. Carignano, M. Lagos, M. Mannarelli and A. Vera,Pion crystals hosting topologically stable baryons,Phys. Rev. D103(2021) 076003 [2012.05921]

  31. [31]

    Canfora, M

    F. Canfora, M. Lagos and A. Vera,Superconducting multi-vortices and a novel BPS bound in chiral perturbation theory,JHEP10(2024) 224 [2405.08082]

  32. [32]

    Evans and A

    G.W. Evans and A. Schmitt,Chiral anomaly induces superconducting baryon crystal,JHEP 09(2022) 192 [2206.01227]

  33. [33]

    Evans and A

    G.W. Evans and A. Schmitt,Chiral Soliton Lattice turns into 3D crystal,JHEP2024(2024) 041 [2311.03880]

  34. [34]

    Skyrme,A Nonlinear field theory,Proc

    T.H.R. Skyrme,A Nonlinear field theory,Proc. Roy. Soc. Lond. A260(1961) 127

  35. [35]

    Skyrme,A Unified Field Theory of Mesons and Baryons,Nucl

    T.H.R. Skyrme,A Unified Field Theory of Mesons and Baryons,Nucl. Phys.31(1962) 556

  36. [36]

    Correspondence between Skyrmions in 2+1 and 3+1 Dimensions

    M. Nitta,Correspondence between Skyrmions in 2+1 and 3+1 Dimensions,Phys. Rev. D87 (2013) 025013 [1210.2233]

  37. [37]

    Matryoshka Skyrmions

    M. Nitta,Matryoshka Skyrmions,Nucl. Phys. B872(2013) 62 [1211.4916]

  38. [38]

    Gudnason and M

    S.B. Gudnason and M. Nitta,Incarnations of Skyrmions,Phys. Rev. D90(2014) 085007 [1407.7210]

  39. [39]

    Gudnason and M

    S.B. Gudnason and M. Nitta,Domain wall Skyrmions,Phys. Rev. D89(2014) 085022 [1403.1245]

  40. [40]

    Eto and M

    M. Eto and M. Nitta,Non-Abelian Sine-Gordon Solitons: Correspondence betweenSU(N) Skyrmions andCP N−1 Lumps,Phys. Rev. D91(2015) 085044 [1501.07038]

  41. [41]

    M. Eto, K. Nishimura and M. Nitta,Domain-Wall Skyrmion Phase in Dense QCD at Strong Magnetic Fields Using Leading-Order Chiral Perturbation Theory,Phys. Rev. Lett.134 (2025) 181902 [2304.02940]

  42. [42]

    M. Eto, K. Nishimura and M. Nitta,Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice,JHEP12(2023) 032 [2311.01112]

  43. [43]

    Amari, M

    Y. Amari, M. Eto and M. Nitta,Domain-wall Skyrmion phase of QCD in magnetic field: gauge field dynamics,JHEP05(2025) 037 [2409.08841]. – 15 –

  44. [44]

    Amari, M

    Y. Amari, M. Nitta and R. Yokokura,Spin statistics and surgeries of topological solitons in QCD matter in magnetic field,JHEP02(2025) 171 [2406.14419]

  45. [45]

    Copinger, M

    P. Copinger, M. Eto, M. Nitta and Z. Qiu,Fermionic domain-wall Skyrmions of QCD in a magnetic field,JHEP (to appear)(2025) [2512.22023]

  46. [46]

    Gudnason and M

    S.B. Gudnason and M. Nitta,Baryonic torii: Toroidal baryons in a generalized Skyrme model,Phys. Rev. D91(2015) 045027 [1410.8407]

  47. [47]

    Gudnason and M

    S.B. Gudnason and M. Nitta,Skyrmions confined as beads on a vortex ring,Phys. Rev. D94 (2016) 025008 [1606.00336]

  48. [48]

    Nitta,Fractional instantons and bions in the principal chiral model onR 2 ×S 1 with twisted boundary conditions,JHEP08(2015) 063 [1503.06336]

    M. Nitta,Fractional instantons and bions in the principal chiral model onR 2 ×S 1 with twisted boundary conditions,JHEP08(2015) 063 [1503.06336]

  49. [49]

    Nitta,Relations among topological solitons,Phys

    M. Nitta,Relations among topological solitons,Phys. Rev. D105(2022) 105006 [2202.03929]

  50. [50]

    Manohar and H

    A. Manohar and H. Georgi,Chiral Quarks and the Nonrelativistic Quark Model,Nucl. Phys. B234(1984) 189

  51. [51]

    Axial anomaly and magnetism of nuclear and quark matter

    D.T. Son and M.A. Stephanov,Axial anomaly and magnetism of nuclear and quark matter, Phys. Rev. D77(2008) 014021 [0710.1084]

  52. [52]

    Goldstone and F

    J. Goldstone and F. Wilczek,Fractional Quantum Numbers on Solitons,Phys. Rev. Lett.47 (1981) 986

  53. [53]

    Adkins, C.R

    G.S. Adkins, C.R. Nappi and E. Witten,Static Properties of Nucleons in the Skyrme Model, Nucl. Phys. B228(1983) 552

  54. [54]

    Gudnason and M

    S.B. Gudnason and M. Nitta,Linking number of vortices as baryon number,Phys. Rev. D 101(2020) 065011 [2002.01762]

  55. [55]

    Gudnason and M

    S.B. Gudnason and M. Nitta,Linked vortices as baryons in the miscible BEC-Skyrme model, Phys. Rev. D102(2020) 045022 [2006.04067]. – 16 –