Zihao Song
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Zihao Song has a total of 9 co-authors. Here are the top co-authors by number of shared publications:
- Jiang Xu
School of Mathematics, Nanjing University of Aeronautics and Astronautics, Nanjing, People’s Republic of China
3 shared publications - Timothée Crin-Barat
Institut de Mathématiques de Toulouse, Université de Toulouse, Toulouse, France
2 shared publications Jiang Xu
School of Mathematics Nanjing University of Aeronautics and Astronautics 211106 Jiangsu Province Nanjing China
1 shared publication- Jianzhong Zhang
Department of Mathematics, Nanjing University of Aeronautics and Astronautics, Nanjing, People’s Republic of China
1 shared publication - Lianchao Gu
School of Mathematics and Key Laboratory of Mathematical MIIT, Nanjing University of Aeronautics and Astronautics, Nanjing, P. R. China
1 shared publication - Ling-Yun Shou
School of Mathematical Sciences, Ministry of Education Key Laboratory of NSLSCS, and Key Laboratory of Jiangsu Provincial Universities of FDMTA, Nanjing Normal University, Nanjing, China
1 shared publication
Latest Publications
- 25 June 2026
- Published by IOP Publishing in Nonlinearity
- Vol. 39 (6) , 065013
Large time behaviors for solutions of the compressible Navier–Stokes system with capillarity
We present a new derivation for the asymptotic behaviors for solutions of the compressible Korteweg system with derivatives of arbitrary high order in general L r ( R d ) ( d ⩾ 2 , r ∈ [ 1 , ∞ ] ). It would be shown that solutions decay at the rates of heat kernels for 2 ⩽ r ⩽ ∞ while decay slower, asymptotically behaving as so called ‘diffusion waves’, for 1 ⩽ r < 2 . By introducing an initial space with negative regularity B ˙ 1 , ∞ − σ , we obtain the uniform decay for solutions within L 1 framework, compared to the possible growth in classical results for compressible models. The approach is so-called Gevrey method, based on the parabolic mechanics of the linearized system, which enables us to transform high order derivatives’ estimates into decay rates and low-order analytic estimates. In order to control the growth of the radius of analyticity under the particular regularity, especially in case 1 ⩽ r < 2 , we shall treat the momentum form of the perturbed system, establish necessary linear analysis based on the semi-group and Gevrey product estimates in sub-analytic families.
- 25 June 2026
- Published by IOP Publishing in Nonlinearity
- Vol. 39 (6) , 065013
Large time behaviors for solutions of the compressible Navier–Stokes system with capillarity
We present a new derivation for the asymptotic behaviors for solutions of the compressible Korteweg system with derivatives of arbitrary high order in general L r ( R d ) ( d ⩾ 2 , r ∈ [ 1 , ∞ ] ). It would be shown that solutions decay at the rates of heat kernels for 2 ⩽ r ⩽ ∞ while decay slower, asymptotically behaving as so called ‘diffusion waves’, for 1 ⩽ r < 2 . By introducing an initial space with negative regularity B ˙ 1 , ∞ − σ , we obtain the uniform decay for solutions within L 1 framework, compared to the possible growth in classical results for compressible models. The approach is so-called Gevrey method, based on the parabolic mechanics of the linearized system, which enables us to transform high order derivatives’ estimates into decay rates and low-order analytic estimates. In order to control the growth of the radius of analyticity under the particular regularity, especially in case 1 ⩽ r < 2 , we shall treat the momentum form of the perturbed system, establish necessary linear analysis based on the semi-group and Gevrey product estimates in sub-analytic families.
- Open Access
Electrostatic effects on critical regularity and long-time behavior of viscous compressible fluids
We consider the compressible Navier-Stokes-Poisson equations in $\mathbb{R}^d$ ($d\geq2$), a classical model for barotropic compressible flows coupled with a self-consistent electrostatic potential. We show that the electrostatic coupling has a significant impact on the long-time dynamics of solutions due to its underlying Klein-Gordon structure. As a first result, we prove the global well-posedness of the Cauchy problem with initial data near equilibrium in the full-frequency $L^{p}$-type critical Besov space \emph{without relying on hyperbolic symmetrization}. Compared with the Poisson-free case studied in several milestone works [Charve and Danchin, Arch. Rational Mech. Anal., 198 (2010), 233-271; Chen, Miao and Zhang, Commun. Pure Appl. Math., 63 (2010), 1173-1224; Haspot, Arch. Rational Mech. Anal., 202 (2011), 427-460], we remove the extra $L^{2}$ assumption in low frequencies and extend the admissible choice of $p$ to the sharp range $1\leq p<2d$. This is, to the best of our knowledge, the first result in compressible fluids that allows the initial velocity field to be highly oscillatory across all frequencies. Furthermore, stemming from the Poisson coupling, the density and velocity exhibit distinct low-frequency behaviors. Motivated by this feature, we propose a general $L^p$-type low-frequency assumption and establish the optimal convergence rates of global solutions toward equilibrium. For a broad class of indices, this assumption yields faster decay than those obtained under the classical $L^1$ framework. To this end, we develop a time-weighted energy method, which is of interest and enables us to capture maximal decay estimates without additional smallness of initial data.Open AccessElectrostatic effects on critical regularity and long-time behavior of viscous compressible fluids
We consider the compressible Navier-Stokes-Poisson equations in $\mathbb{R}^d$ ($d\geq2$), a classical model for barotropic compressible flows coupled with a self-consistent electrostatic potential. We show that the electrostatic coupling has a significant impact on the long-time dynamics of solutions due to its underlying Klein-Gordon structure. As a first result, we prove the global well-posedness of the Cauchy problem with initial data near equilibrium in the full-frequency $L^{p}$-type critical Besov space \emph{without relying on hyperbolic symmetrization}. Compared with the Poisson-free case studied in several milestone works [Charve and Danchin, Arch. Rational Mech. Anal., 198 (2010), 233-271; Chen, Miao and Zhang, Commun. Pure Appl. Math., 63 (2010), 1173-1224; Haspot, Arch. Rational Mech. Anal., 202 (2011), 427-460], we remove the extra $L^{2}$ assumption in low frequencies and extend the admissible choice of $p$ to the sharp range $1\leq p<2d$. This is, to the best of our knowledge, the first result in compressible fluids that allows the initial velocity field to be highly oscillatory across all frequencies. Furthermore, stemming from the Poisson coupling, the density and velocity exhibit distinct low-frequency behaviors. Motivated by this feature, we propose a general $L^p$-type low-frequency assumption and establish the optimal convergence rates of global solutions toward equilibrium. For a broad class of indices, this assumption yields faster decay than those obtained under the classical $L^1$ framework. To this end, we develop a time-weighted energy method, which is of interest and enables us to capture maximal decay estimates without additional smallness of initial data. - Open Access
The compressible Euler system with damping in hybrid Besov spaces: global well-posedness and relaxation limit
We investigate the global well-posedness of the compressible Euler system with damping in R^d (d ≥ 1) and its relaxation limit toward the porous medium equation. In [12], the first author and Danchin studied these two problems in hybrid Besov spaces, where the high-frequency components of the solution are bounded in L2 -based norms, while the lowfrequency components are controlled in L p -based norms with p ∈ [2, max{4, 2d/(d -2)}]. Motivated by the observation that the limit system is well-posed in Lp -based spaces for p ∈ [2, ∞), we extend the low-frequency analysis to this full range, thereby providing a more unified framework for studying such relaxation limits.The core of our proof consists in establishing refined product and commutator estimates describing sharply the interactions between the high, medium, and low-frequency regimes. A key observation underlying our analysis is that the product of two functions localized at low frequencies generates only interactions between low and medium frequencies, never purely high-frequency ones. Consequently, for a suitable choice of frequency threshold, the high-frequency projection of the product of two functions localized low frequencies vanishes.
Open AccessThe compressible Euler system with damping in hybrid Besov spaces: global well-posedness and relaxation limit
We investigate the global well-posedness of the compressible Euler system with damping in R^d (d ≥ 1) and its relaxation limit toward the porous medium equation. In [12], the first author and Danchin studied these two problems in hybrid Besov spaces, where the high-frequency components of the solution are bounded in L2 -based norms, while the lowfrequency components are controlled in L p -based norms with p ∈ [2, max{4, 2d/(d -2)}]. Motivated by the observation that the limit system is well-posed in Lp -based spaces for p ∈ [2, ∞), we extend the low-frequency analysis to this full range, thereby providing a more unified framework for studying such relaxation limits.The core of our proof consists in establishing refined product and commutator estimates describing sharply the interactions between the high, medium, and low-frequency regimes. A key observation underlying our analysis is that the product of two functions localized at low frequencies generates only interactions between low and medium frequencies, never purely high-frequency ones. Consequently, for a suitable choice of frequency threshold, the high-frequency projection of the product of two functions localized low frequencies vanishes.
- Open Access
The compressible Euler system with damping in hybrid Besov spaces: global well-posedness and relaxation limit
We investigate the global well-posedness of the compressible Euler system with damping in Rd (d\geq1) and its relaxation limit toward the porous medium equation. In [12], the first author and Danchin studied these two problems in hybrid Besov spaces, where the high-frequency components of the solution are bounded in L2-based norms, while the low-frequency components are controlled in Lp-based norms with p\in[2,\max{4,\frac{2d}{d-2}}]. Motivated by the observation that the limit system is well-posed in Lp-based spaces for p\in[2, \infty), we extend the low-frequency analysis to this full range, thereby providing a more unified framework for studying such relaxation limits. The core of our proof consists in establishing refined product and commutator estimates describing sharply the interactions between the high, medium, and low-frequency regimes. A key observation underlying our analysis is that the product of two functions localized at low frequencies generates only interactions between low and medium frequencies, never purely high-frequency ones. Consequently, for a suitable choice of frequency threshold, the high-frequency projection of the product of two functions localized low frequencies vanishes.
Open AccessThe compressible Euler system with damping in hybrid Besov spaces: global well-posedness and relaxation limit
We investigate the global well-posedness of the compressible Euler system with damping in Rd (d\geq1) and its relaxation limit toward the porous medium equation. In [12], the first author and Danchin studied these two problems in hybrid Besov spaces, where the high-frequency components of the solution are bounded in L2-based norms, while the low-frequency components are controlled in Lp-based norms with p\in[2,\max{4,\frac{2d}{d-2}}]. Motivated by the observation that the limit system is well-posed in Lp-based spaces for p\in[2, \infty), we extend the low-frequency analysis to this full range, thereby providing a more unified framework for studying such relaxation limits. The core of our proof consists in establishing refined product and commutator estimates describing sharply the interactions between the high, medium, and low-frequency regimes. A key observation underlying our analysis is that the product of two functions localized at low frequencies generates only interactions between low and medium frequencies, never purely high-frequency ones. Consequently, for a suitable choice of frequency threshold, the high-frequency projection of the product of two functions localized low frequencies vanishes.
- 12 January 2026
- Published by Springer Nature in Calculus of Variations and Partial Differential Equations
- Vol. 65 (2) , 58
Global dynamics of the quantum Euler system with damping in the critical space
- 12 January 2026
- Published by Springer Nature in Calculus of Variations and Partial Differential Equations
- Vol. 65 (2) , 58
Global dynamics of the quantum Euler system with damping in the critical space
- Open Access
Global well-posedness for the 3D compressible Navier-Stokes equations in optimal Besov space
We consider the Cauchy problem to the 3D barotropic compressible Navier-Stokes equation. We prove global well-posedness, assuming that the initial data $(ρ_0-1,u_0)$ has small norms in the critical Besov space $\mathbb{X}_p=\dot{B}_{p,1}^{3/p}(\mathbb{R}^3)\times \dot{B}_{p,1}^{-1+3/p}(\mathbb{R}^3)$ for $2\leq p<6$ and $(ρ_0-1,ρ_0u_0)$ satisfies an additional low frequency condition. Our results extend the previous results in \cite{FD2010, CMZ2010, H20112} where $p<4$ is needed for high frequency, to the optimal range $p<6$. The main ingredients of the proof consist of: a novel nonlinear transform that uses momentum formulation for low-frequency and effective velocity method for high frequency, and estimate of parabolic-dispersive semigroup that enables a $L^q$-framework for low frequency.Open AccessGlobal well-posedness for the 3D compressible Navier-Stokes equations in optimal Besov space
We consider the Cauchy problem to the 3D barotropic compressible Navier-Stokes equation. We prove global well-posedness, assuming that the initial data $(ρ_0-1,u_0)$ has small norms in the critical Besov space $\mathbb{X}_p=\dot{B}_{p,1}^{3/p}(\mathbb{R}^3)\times \dot{B}_{p,1}^{-1+3/p}(\mathbb{R}^3)$ for $2\leq p<6$ and $(ρ_0-1,ρ_0u_0)$ satisfies an additional low frequency condition. Our results extend the previous results in \cite{FD2010, CMZ2010, H20112} where $p<4$ is needed for high frequency, to the optimal range $p<6$. The main ingredients of the proof consist of: a novel nonlinear transform that uses momentum formulation for low-frequency and effective velocity method for high frequency, and estimate of parabolic-dispersive semigroup that enables a $L^q$-framework for low frequency. - 9 April 2025
- Published by Springer Nature in Mathematische Annalen
- Vol. 392 (2) , 2157-2224
Global dynamics and vanishing capillarity limit of the 3D Euler–Poisson–Korteweg equations
- 9 April 2025
- Published by Springer Nature in Mathematische Annalen
- Vol. 392 (2) , 2157-2224
Global dynamics and vanishing capillarity limit of the 3D Euler–Poisson–Korteweg equations
- 18 July 2024
- Published by Elsevier in Journal of Mathematical Analysis and Applications
- Vol. 541 (2)
Decay of higher order derivatives for L solutions to the compressible fluid model of Korteweg type
- 18 July 2024
- Published by Elsevier in Journal of Mathematical Analysis and Applications
- Vol. 541 (2)
Decay of higher order derivatives for L solutions to the compressible fluid model of Korteweg type
- 26 April 2024
- Published by Springer Nature in Calculus of Variations and Partial Differential Equations
- Vol. 63 (5) , 1-30
Global dynamics of large solution for the compressible Navier–Stokes–Korteweg equations
- 26 April 2024
- Published by Springer Nature in Calculus of Variations and Partial Differential Equations
- Vol. 63 (5) , 1-30
Global dynamics of large solution for the compressible Navier–Stokes–Korteweg equations
- Open Access
Global dynamics of Kato's solutions for the 3D incompressible micropolar system
We consider the global well-posedness and decay rates for solutions of 3D incompressible micropolar equation in the critical Besov space. Spectrum analysis allows us to find not only parabolic behaviors of solutions, but also damping effect of angular velocity in the low frequencies. Based on this observation, we establish the global well-posedness with more general regularity on the initial data. The approach concerns large time behaviors is so-called the Gevrey method which bases on the parabolic mechanics of the micropolar system. This method enables us even to derive decay of \textit{arbitrary} higher order derivatives by transforming it into the control of the radius of analyticity under a particular regularity. To bound the growth of the radius of analyticity in general $L^p$ Besov spaces, we shall develop some new techniques concern Gevrey estimates, especially an extended Coifman-Meyer theory, to cover those endpoint Lebesgue framework.Open AccessGlobal dynamics of Kato's solutions for the 3D incompressible micropolar system
We consider the global well-posedness and decay rates for solutions of 3D incompressible micropolar equation in the critical Besov space. Spectrum analysis allows us to find not only parabolic behaviors of solutions, but also damping effect of angular velocity in the low frequencies. Based on this observation, we establish the global well-posedness with more general regularity on the initial data. The approach concerns large time behaviors is so-called the Gevrey method which bases on the parabolic mechanics of the micropolar system. This method enables us even to derive decay of \textit{arbitrary} higher order derivatives by transforming it into the control of the radius of analyticity under a particular regularity. To bound the growth of the radius of analyticity in general $L^p$ Besov spaces, we shall develop some new techniques concern Gevrey estimates, especially an extended Coifman-Meyer theory, to cover those endpoint Lebesgue framework.