Searcharxiv⌕ Search

arXiv · 2610.26958

Linear Structure, Convergence and Resurgence of Hydrodynamic Transseries

Abstract

We construct an exact formulation for the solution of Bjorken expanding relativistic viscous hydrodynamics with a constant relaxation time and derive its late time transseries structure. The two fundamental modes of the linear auxiliary equation separate the hydrodynamic contribution from the exponentially suppressed transient mode. We show that this single transient mode generates the entire hierarchy of nonperturbative sectors through nonlinear mode mixing, while its decay explains the loss of initial condition dependence and the emergence of late time hydrodynamic attractor behavior. The hydrodynamic gradient expansion is factorially divergent for generic values of the transport parameter but converges at the discrete values $a=N^2$, where the auxiliary asymptotic expansions terminate. We further determine the exact Stokes constant of the auxiliary linear equation and establish its relation to the logarithmic Borel singularity coefficient. The vanishing of the Stokes constant at these exceptional values establishes a direct connection between auxiliary series termination, hydrodynamic convergence, and Stokes decoupling between the hydrodynamic and the nonhydrodynamic transient sector.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Qi Zhou, Enke Wang, Hui Zhang. 2026-10-18. Linear Structure, Convergence and Resurgence of Hydrodynamic Transseries. https://arxiv.org/abs/2610.26958

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Orientation effects of deformed nuclei in intermediate-energy nuclear scattering

We investigate the effects of nuclear deformation on intermediate-energy nuclear scattering within the Glauber theory. A formalism that explicitly incorporates the orientation dependence of deformed intrinsic states is derived, in which reaction observables are first computed with a fixed orientation and then the angle average of the reaction observables is taken afterwards. This formalism is applied to elastic scattering and total reaction cross sections. In addition, a new expansion scheme of the optical-limit approximation is proposed and shown to include contributions from a class of nuclear excitations, allowing a simple estimate of part of the total inelastic scattering cross section. The orientation dependence is generally weak for both proton- and carbon-target scattering and supports the validity of conventional treatments with an angle averaged density for light and medium-heavy nuclei. However, noticeable deviations emerge for strongly deformed heavy nuclei. The present analysis further demonstrates that the summed inelastic scattering cross section to rotationally excited states can be interpreted as a manifestation of fluctuations of the nuclear surface density associated with deformation. The present study provides a quantum-mechanical interpretation of deformation effects in intermediate-energy nuclear reactions and suggests a pathway toward a more reliable theoretical description of interaction cross section measurements. Brief comments on the role of nuclear deformation in low-energy heavy-ion reactions and ultra-relativistic heavy-ion collisions are also made.

nucl-th↗

Numerical study of the three-boson bound-state problem in partial-wave and vector-variable formulations

We present a systematic benchmark of the three-boson bound-state problem in momentum space, comparing one-dimensional (1D) spectator-amplitude, two-dimensional (2D) partial-wave, and three-dimensional (3D) vector-variable formulations. The benchmark controls the interaction representation by embedding the same finite partial-wave interaction space in each formulation, so that discrepancies reflect discretization, interpolation, and quadrature errors. This enables direct 1D--2D--3D comparisons for separable interactions, controlled 2D--3D tests for local interactions, and comparison with the full local interaction in the 3D vector-variable formulation. Binding energies agree at the $10^{-6}$~MeV level for the separable interactions. For the local interactions at $l_{\rm max}=12$, the 2D--3D differences are $2.2\times10^{-6}$~MeV for MT-V and $5.3\times10^{-5}$~MeV for MT-IV. The 2D and 3D equations are also solved in both $t$-matrix-driven and bare-potential-driven forms, whose agreement validates the permutation geometry, quadrature, and interpolation. Fourier transforms to coordinate space yield consistent norm decompositions and spatial observables, providing an independent check of the momentum-space solutions.

nucl-th↗

Transport simulations with a constrained momentum-dependent chiral mean-field equation of state at various isospin fractions

We present a comparison of the UrQMD model using a chiral mean field EoS (CMF) with flow and pion production data in heavy ion collisions at low beam energies $E_{\mathrm{lab}}=0.2-2.0 A$ GeV and varying iso-spin fraction. The CMF model parameters are constrained by known properties of the high density equation of state of QCD at varying iso-spin fractions. This allows us to calculate the equation of state as well as nuclear interactions for different physical systems like neutron stars and heavy ion collisions in a consistent way. It is found that heavy ion reactions at the upcoming FAIR facility will only have marginal sensitivity on the iso-spin dependence of the high-density equation of state. At lower beam energies, comparing to FOPI, HADES and S$π$rit data, the sensitivity is higher but the observed deviations and systematic uncertainties of the existing data are larger than the sensitivity to the symmetry energy.

nucl-th↗