Global Well-posedness and Regularity of the Dynamical Prandtl Equation
Pith reviewed 2026-06-27 06:10 UTC · model grok-4.3
The pith
The dynamical Prandtl equation has global classical solutions under a monotonicity condition on the data.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using a precise description of the fundamental solution to the Kolmogorov equation in the half-space, the authors obtain the Holder regularity of local weak solutions up-to-boundary. They then use this together with Hormander's hypoelliptic estimates to prove higher-order regularity and establish global existence and regularity of classical solutions to the dynamical Prandtl equation under monotonicity assumptions. The same estimates also yield a self-contained local existence theory via weighted energy estimates and expand the theory of global weak solutions while incorporating all physical types of asymptotic matching.
What carries the argument
Precise description of the fundamental solution to the Kolmogorov equation in the half-space, which supplies the up-to-boundary Holder estimates for weak solutions in Crocco coordinates.
If this is right
- Global classical solutions exist for the dynamical Prandtl equation whenever the data satisfy the monotonicity condition.
- Up-to-boundary smoothness in Crocco coordinates transfers to smoothness of the Prandtl solutions in the original physical variables.
- The local existence theory holds via weighted energy estimates without relying on prior local classical constructions.
- Global weak solutions can be constructed that incorporate all physical types of boundary-layer matching with the outer flow.
- Higher-order regularity follows from the boundary Holder estimates combined with hypoelliptic regularity theory.
Where Pith is reading between the lines
- The same half-space Kolmogorov fundamental solution technique could be tested on related hypoelliptic boundary-value problems arising in other fluid models.
- If the monotonicity condition can be relaxed while keeping the fundamental-solution description, the method might extend to a larger class of initial data for the vanishing-viscosity problem.
- The up-to-boundary regularity result supplies a concrete starting point for numerical schemes that aim to resolve the boundary layer without interior-only smoothing.
Load-bearing premise
The fundamental solution of the Kolmogorov equation in the half-space has a description precise enough to produce up-to-boundary Holder estimates for the weak solutions.
What would settle it
A monotonicity-satisfying initial datum whose corresponding Prandtl solution develops a singularity in finite time, or a concrete failure of the Kolmogorov fundamental solution description to deliver the claimed Holder regularity.
read the original abstract
In this paper, we study the dynamical Prandtl equation, which plays an important role in the study of the vanishing viscosity limit of the Navier--Stokes equations. Our focus is on the (Sobolev) well-posedness regime, where the given data satisfy a crucial monotonicity condition. In this case, local classical solutions have been constructed in the pioneering works of Oleinik \cite{O68,OS99}. More recently, global weak solutions were obtained in \cite{XZ04} by Xin and Zhang, and in \cite{XZZ24} by Xin, Zhang, and Zhao, where the uniqueness and interior H"older estimates of the solutions were established (in Crocco coordinates). Using a precise description of the fundamental solution to the Kolmogorov equation in the half-space, we first obtain the H"older regularity of local weak solutions up-to-boundary. We also provide a detailed proof of higher-order regularity estimates using this H"older regularity, together with H"ormander's hypoelliptic estimates, which are nontrivial. Up-to-boundary smoothness of solutions (in Crocco coordinates) is important in order to conclude the smoothness of the Prandtl solutions in the physical variables, even in the interior. It is also physically significant for applications to the Boundary Layer Theory where the dynamical Prandtl equation is essential. Using these smoothing estimates, we then prove the global existence and regularity of classical solutions to the dynamical Prandtl equation under monotonicity assumptions, which was listed by Oleinik and Samokhin in \cite{OS99} as one of the open problems. We also develop a self-contained local existence theory using weighted energy estimates and further expand the theory of global weak solutions. The main point is to incorporate all physical types of asymptotic matching of the boundary layer with the outer flow, which is expected to be useful for applications to the Navier--Stokes equations.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims global well-posedness and regularity of classical solutions to the dynamical Prandtl equation under monotonicity assumptions. It proceeds by deriving up-to-boundary Hölder regularity for local weak solutions from a precise description of the fundamental solution to the Kolmogorov equation in the half-space, bootstrapping to higher regularity via Hörmander hypoelliptic estimates, and then using these smoothing properties to obtain global classical solutions; a self-contained local existence theory via weighted energy estimates is also developed, along with an expansion of the global weak-solution theory that incorporates all physical types of asymptotic matching.
Significance. If the up-to-boundary Hölder estimates hold uniformly, the result would resolve the open problem of global classical solutions listed in Oleinik-Samokhin (OS99), completing the well-posedness theory in the monotonicity regime and supplying the boundary smoothness in Crocco coordinates needed to recover smoothness in physical variables. The incorporation of weighted estimates and multiple asymptotic matchings strengthens applicability to the vanishing-viscosity limit for Navier-Stokes.
major comments (2)
- [Abstract / Hölder regularity section] Abstract (Hölder regularity paragraph) and the section deriving boundary estimates from the Kolmogorov fundamental solution: the claim that the precise description yields Hölder regularity up-to-boundary must be accompanied by explicit constants and estimates that remain uniform as dist(x,∂)→0; without this uniformity the subsequent global continuation argument and the return map from Crocco to physical variables cannot close, as both rely on controlling the boundary trace.
- [Higher-order regularity section] The passage from Hölder regularity to higher-order estimates via Hörmander hypoelliptic estimates (the paragraph beginning 'We also provide a detailed proof of higher-order regularity estimates'): the argument must verify that the hypoelliptic constants do not deteriorate near the boundary once the Hölder modulus is only known up to the boundary; any loss of uniformity here would block the smoothness needed for the global existence theorem.
minor comments (2)
- [Abstract] The abstract refers to 'H"older' and 'H"ormander' with inconsistent escaping; standardize the diacritics throughout.
- [References] The citation list includes [XZZ24] but the text does not clarify whether this is a preprint or published version; add the full bibliographic data.
Simulated Author's Rebuttal
We thank the referee for the detailed and insightful report. The comments highlight important points regarding uniformity of estimates near the boundary, which are essential for closing the global existence argument and recovering physical-variable regularity. We address each major comment below and will revise the manuscript to strengthen the presentation of uniformity.
read point-by-point responses
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Referee: [Abstract / Hölder regularity section] Abstract (Hölder regularity paragraph) and the section deriving boundary estimates from the Kolmogorov fundamental solution: the claim that the precise description yields Hölder regularity up-to-boundary must be accompanied by explicit constants and estimates that remain uniform as dist(x,∂)→0; without this uniformity the subsequent global continuation argument and the return map from Crocco to physical variables cannot close, as both rely on controlling the boundary trace.
Authors: We agree that explicit uniformity is required to justify the global continuation and the Crocco-to-physical change of variables. The fundamental solution of the Kolmogorov equation in the half-space is constructed via an explicit parametrix that incorporates the boundary condition through reflection and Gaussian decay in the normal variable; the resulting Hölder modulus is controlled by constants depending only on the monotonicity lower bound and the L^∞ norm of the data, both of which are independent of distance to the boundary. In the revision we will add a dedicated lemma (new Lemma 3.4) that extracts the explicit constants from the parametrix representation and verifies that they remain bounded as dist(x,∂)→0, thereby closing the estimates used in the global existence theorem. revision: yes
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Referee: [Higher-order regularity section] The passage from Hölder regularity to higher-order estimates via Hörmander hypoelliptic estimates (the paragraph beginning 'We also provide a detailed proof of higher-order regularity estimates'): the argument must verify that the hypoelliptic constants do not deteriorate near the boundary once the Hölder modulus is only known up to the boundary; any loss of uniformity here would block the smoothness needed for the global existence theorem.
Authors: We acknowledge that the hypoelliptic constants must be shown not to blow up at the boundary. The Hörmander estimates are applied after the uniform Hölder modulus has already been established up to the boundary; the vector fields satisfy the Hörmander condition uniformly because the coefficients remain bounded and the monotonicity prevents degeneracy at the boundary. In the revision we will insert a short paragraph (after the current display (4.12)) that tracks the dependence of the hypoelliptic constants on the Hölder modulus and confirms that they stay controlled by quantities independent of distance to the boundary, using the same parametrix estimates already derived for the first-order regularity. revision: yes
Circularity Check
No significant circularity; direct analytic derivation from external inputs
full rationale
The paper's chain begins from prior local classical solutions (Oleinik) and global weak solutions with interior estimates (Xin-Zhang et al.), then claims to derive up-to-boundary Hölder regularity from an independent description of the Kolmogorov fundamental solution in the half-space, followed by Hörmander hypoelliptic estimates for higher regularity and global classical existence under monotonicity. No step reduces the target result to a fitted parameter, self-defined quantity, or load-bearing self-citation by construction; the central global well-posedness statement remains independent of the paper's own outputs. The derivation is therefore self-contained against the stated external starting points and analytic tools.
Axiom & Free-Parameter Ledger
axioms (2)
- standard math Existence and basic properties of the fundamental solution to the Kolmogorov equation in the half-space
- standard math Hormander's hypoelliptic regularity theory applies once Holder continuity is established
Reference graph
Works this paper leans on
-
[1]
Alexandre, Y
R. Alexandre, Y. Wang, C. Xu, and T. Yang. Well-posedness of the Prandtl equation in Sobolev spaces. J. Amer. Math. Soc. , 28(3):745–784, 2015
2015
-
[2]
Bahouri, J
H. Bahouri, J. Chemin, and R. Danchin. Fourier analysis and nonlinear partial differential equatio ns, volume 343 of Grundlehren der mathematischen Wissenschaften . Springer, Heidelberg, 2011
2011
-
[3]
grenzschichten in ߬ ussigkeiten mit klein er reibung
H. Blasius. “grenzschichten in fl¨ ussigkeiten mit klein er reibung”. Z. Angew. Math. Phys. , pages 1–37, 1908
1908
-
[4]
J. Bony. Principe du maximum, in´ egalite de Harnack et un icit´ e du probl` eme de Cauchy pour les op´ erateurs elliptiques d´ eg´ en´ er´ es.Ann. Inst. Fourier (Grenoble) , 19:277–304 xii, 1969
1969
-
[5]
F. Bouchut. Hypoelliptic regularity in kinetic equatio ns. J. Math. Pures Appl. (9) , 81(11):1135–1159, 2002
2002
-
[6]
Bramanti and M
M. Bramanti and M. Cerutti. Commutators of singular inte grals on homogeneous spaces. Boll. Un. Mat. Ital. B (7) , 10(4):843–883, 1996
1996
-
[7]
Bramanti, M
M. Bramanti, M. Cerutti, and M. Manfredini. lp estimates for some ultraparabolic operators with discon- tinuous coefficients. J. Math. Anal. Appl. , 200(2):332–354, 1996
1996
-
[8]
H. Brezis. On a conjecture of J. Serrin. Atti Accad. Naz. Lincei Cl. Sci. Fis. Mat. Natur. , 19:335–338, 2008
2008
-
[9]
G. Chen and C. Zhao. Sharp asymptotic behavior of the stea dy pressure-free Prandtl system. arXiv preprint arXiv:2504.11870, 2025
arXiv 2025
-
[10]
Coifman and M
R. Coifman and M. Guzm´ an. Singular integrals and multi pliers on homogeneous spaces. Rev. Un. Mat. Argentina, 25:137–143, 1970/71
1970
-
[11]
Coifman and G
R. Coifman and G. Weiss. Analyse harmonique non-commutative sur certains espaces h omog` enes, volume Vol. 242 of Lecture Notes in Mathematics . Springer-Verlag, Berlin-New York, 1971
1971
-
[12]
Collot, T
C. Collot, T. Ghoul, S. Ibrahim, and N. Masmoudi. On sing ularity formation for the two-dimensional unsteady Prandtl system around the axis. J. Eur. Math. Soc. (JEMS) , 24(11):3703–3800, 2022
2022
-
[13]
L. Crocco. Sullo strato limite laminare nei gas lungo un a lamina plana. Rend. Math. Appl. Ser. 5 , 21:2:484– 491, 1941
1941
-
[14]
Dalibard and N
A. Dalibard and N. Masmoudi. Separation for the station ary Prandtl equation. Publ. Math. Inst. Hautes ´Etudes Sci. , 130:187–297, 2019
2019
-
[15]
Sulla differenziabilit` a e l’analitic it` a delle estremali degli integrali multipli regolari
Ennio De Giorgi. Sulla differenziabilit` a e l’analitic it` a delle estremali degli integrali multipli regolari. Mem. Accad. Sci. Torino. Cl. Sci. Fis. Mat. Nat. (3) , 3:25–43, 1957
1957
-
[16]
Dietert and D
H. Dietert and D. G´ erard-Varet. Well-posedness of thePrandtl equations without any structural assumption. Ann. PDE , 5(1):Paper No. 8, 51, 2019
2019
-
[17]
W. E and B. Engquist. Blowup of solutions of the unsteady Prandtl’s equation. Comm. Pure Appl. Math. , 50(12):1287–1293, 1997
1997
-
[18]
Gao and Z
C. Gao and Z. Xin. Prandtl boundary layers in an infinitel y long convergent channel. Comm. Math. Phys. , 407(2):Paper No. 26, 69, 2026
2026
-
[19]
Gao and L
C. Gao and L. Zhang. On the steady prandtl boundary layer expansions. Science China Mathematics , 66:1993–2020, 2023
1993
-
[20]
G´ erard-Varet and E
D. G´ erard-Varet and E. Dormy. On the ill-posedness of t he Prandtl equation. J. Amer. Math. Soc. , 23(2):591–609, 2010
2010
-
[21]
Gerard-Varet and N
D. Gerard-Varet and N. Masmoudi. Well-posedness for th e Prandtl system without analyticity or mono- tonicity. Ann. Sci. ´Ec. Norm. Sup´ er. (4), 48(6):1273–1325, 2015
2015
-
[22]
Golse, C
F. Golse, C. Imbert, C. Mouhot, and A. Vasseur. Harnack i nequality for kinetic Fokker-Planck equations with rough coefficients and application to the Landau equatio n. Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) , 19(1):253–295, 2019
2019
-
[23]
Grafakos
L. Grafakos. Classical Fourier analysis , volume 249 of Graduate Texts in Mathematics . Springer, New York, second edition, 2008
2008
-
[24]
Guerand and C
J. Guerand and C. Imbert. Log-transform and the weak Har nack inequality for kinetic Fokker-Planck equations. J. Inst. Math. Jussieu , 22(6):2749–2774, 2023
2023
-
[25]
Guo and S
Y. Guo and S. Iyer. Regularity and expansion for steady P randtl equations. Comm. Math. Phys. , 382(3):1403–1447, 2021
2021
-
[26]
Guo and T
Y. Guo and T. Nguyen. A note on Prandtl boundary layers. Comm. Pure Appl. Math. , 64(10):1416–1438, 2011
2011
-
[27]
Y. Guo, Y. Wang, and Z. Zhang. Dynamic stability for stea dy Prandtl solutions. Ann. PDE , 9(2):Paper No. 16, 33, 2023
2023
-
[28]
B. Helffer and J. Sjoestrand. From resolvent bounds to se migroup bounds. arXiv preprint arXiv:1001.4171, 2010
Pith/arXiv arXiv 2010
-
[29]
Helffer and J
B. Helffer and J. Sj¨ ostrand. Improving semigroup bound s with resolvent estimates. Integral Equations Op- erator Theory, 93(3):paper no. 36, 41, 2021. 93
2021
-
[30]
E. Hopf. A remark on linear elliptic differential equati ons of second order. Proc. Amer. Math. Soc. , 3:791– 793, 1952
1952
-
[31]
H¨ ormander
L. H¨ ormander. Hypoelliptic second order differential equations. Acta Math. , 119:147–171, 1967
1967
-
[32]
Ignatova and V
M. Ignatova and V. Vicol. Almost global existence for th e Prandtl boundary layer equations. Arch. Ration. Mech. Anal. , 220(2):809–848, 2016
2016
-
[33]
Imbert and C
C. Imbert and C. Mouhot. The Schauder estimate in kineti c theory with application to a toy nonlinear model. Ann. H. Lebesgue , 4:369–405, 2021
2021
-
[34]
S. Iyer. On global-in- x stability of Blasius profiles. Arch. Ration. Mech. Anal. , 237(2):951–998, 2020
2020
-
[35]
S. Iyer and N. Masmoudi. Reversal in the stationary pran dtl equations. arXiv preprint arXiv:2203.02845
-
[36]
Iyer and N
S. Iyer and N. Masmoudi. Global inviscid limit of 2D, sta tionary Navier-Stokes and stability of Prandtl expansions. Forum of Mathematics, Pi , 14:e13, 2026
2026
-
[37]
H. Jia. Uniform linear inviscid damping and enhanced di ssipation near monotonic shear flows in high Reynolds number regime (I): The whole space case. J. Math. Fluid Mech. , 25(3):Paper No. 42, 38, 2023
2023
-
[38]
H. Jia, Z. Lei, and C. Yuan. Sharp asymptotic stability o f Blasius profile in the steady Prandtl equation. Adv. Math. , 480:Paper No. 110533, 65, 2025
2025
-
[39]
Kogoj and E
A. Kogoj and E. Lanconelli. An invariant Harnack inequa lity for a class of hypoelliptic ultraparabolic equations. Mediterr. J. Math. , 1(1):51–80, 2004
2004
-
[40]
S. Kruzkov. A priori bounds and some properties of solut ions of elliptic and parabolic equations. Mat. Sb. (N.S.), 65(107):522–570, 1964
1964
-
[41]
Kukavica, V
I. Kukavica, V. Vicol, and F. Wang. The van Dommelen and S hen singularity in the Prandtl equations. Adv. Math. , 307:288–311, 2017
2017
-
[42]
Lanconelli and S
E. Lanconelli and S. Polidoro. On a class of hypoellipti c evolution operators. Rend. Sem. Mat. Univ. Politec. Torino, 52(1):29–63, 1994. Partial differential equations, II (Tu rin, 1993)
1994
-
[43]
W. Li, D. Wu, and C. Xu. Gevrey class smoothing effect for t he Prandtl equation. SIAM J. Math. Anal. , 48(3):1672–1726, 2016
2016
-
[44]
Li and T
W. Li and T. Yang. Well-posedness in Gevrey function spa ces for the Prandtl equations with non-degenerate critical points. J. Eur. Math. Soc. (JEMS) , 22(3):717–775, 2020
2020
-
[45]
Lions and E
J. Lions and E. Magenes. Non-homogeneous boundary value problems and applications . Vol. II , volume Band 182 of Die Grundlehren der mathematischen Wissenschaften . Springer-Verlag, New York-Heidelberg,
-
[46]
Translated from the French by P. Kenneth
-
[47]
Liu and T
C. Liu and T. Yang. Ill-posedness of the Prandtl equatio ns in Sobolev spaces around a shear flow with general decay. J. Math. Pures Appl. (9) , 108(2):150–162, 2017
2017
-
[48]
Lombardo, M
M. Lombardo, M. Cannone, and M. Sammartino. Well-posed ness of the boundary layer equations. SIAM J. Math. Anal. , 35(4):987–1004, 2003
2003
-
[49]
Masmoudi and T
N. Masmoudi and T. Wong. Local-in-time existence and un iqueness of solutions to the Prandtl equations by energy methods. Comm. Pure Appl. Math. , 68(10):1683–1741, 2015
2015
-
[50]
J. Nash. Continuity of solutions of parabolic and ellip tic equations. Amer. J. Math. , 80:931–954, 1958
1958
-
[51]
Nirenberg
L. Nirenberg. A strong maximum principle for parabolic equations. Comm. Pure Appl. Math. , 6:167–177, 1953
1953
-
[52]
O. A. Oleinik. On properties of solutions of certain bou ndary problems for equations of elliptic type. Mat. Sbornik N.S. , 30/72:695–702, 1952
1952
-
[53]
O. A. Oleinik. Mathematical problems of boundary layer theory. Uspehi Mat. Nauk , 23(3(141)):3–65, 1968
1968
-
[54]
O. A. Oleinik and V. N. Samokhin. Mathematical models in boundary layer theory , volume 15 of Applied Mathematics and Mathematical Computation . Chapman & Hall/CRC, Boca Raton, FL, 1999
1999
-
[55]
Paicu and P
M. Paicu and P. Zhang. Global existence and the decay of s olutions to the Prandtl system with small analytic data. Arch. Ration. Mech. Anal. , 241(1):403–446, 2021
2021
-
[56]
Pascucci and S
A. Pascucci and S. Polidoro. The Moser’s iterative meth od for a class of ultraparabolic equations. Commun. Contemp. Math. , 6(3):395–417, 2004
2004
-
[57]
L. Prandtl. Uber flussigkeits-bewegung bei sehr kleine r reibung. Verhandlungen des III Internationalen Mathematiker-Kongresses, Heidelberg, pages 484–491, 1904
1904
-
[58]
Sammartino and R
M. Sammartino and R. Caflisch. Zero viscosity limit for a nalytic solutions, of the Navier-Stokes equation on a half-space. I. Existence for Euler and Prandtl equation s. Comm. Math. Phys. , 192(2):433–461, 1998
1998
-
[59]
Sammartino and R
M. Sammartino and R. Caflisch. Zero viscosity limit for a nalytic solutions of the Navier-Stokes equation on a half-space. II. Construction of the Navier-Stokes soluti on. Comm. Math. Phys. , 192(2):463–491, 1998
1998
-
[60]
J. Serrin. Pathological solutions of elliptic differen tial equations. Annali della Scuola Normale Superiore di Pisa - Classe di Scienze, Serie 3 , 18:385–387, 1964
1964
-
[61]
J. Serrin. Asymptotic behavior of velocity profiles in t he Prandtl boundary layer theory. Proc. Roy. Soc. London Ser. A , 299:491–507, 1967. 94
1967
-
[62]
W. Shen, Y. Wang, and Z. Zhang. Boundary layer separatio n and local behavior for the steady Prandtl equation. Adv. Math. , 389:Paper No. 107896, 25, 2021
2021
-
[63]
E. Stein. Singular integrals and differentiability properties of func tions, volume No. 30 of Princeton Mathe- matical Series . Princeton University Press, Princeton, NJ, 1970
1970
-
[64]
E. Stein. Harmonic analysis: real-variable methods, orthogonality , and oscillatory integrals , volume 43 of Princeton Mathematical Series . Princeton University Press, Princeton, NJ, 1993
1993
-
[65]
K. Taira. Diffusion processes and partial differential equations . Academic Press, Inc., Boston, MA, 1988
1988
-
[66]
van Dommelen and S
L. van Dommelen and S. Shen. The spontaneous generation of the singularity in a separating laminar boundary layer. Journal of Computational Physics , 38(2):125–140, 1980
1980
-
[67]
C. Wang, Y. Wang, and P. Zhang. On the global small soluti on of 2-D Prandtl system with initial data in the optimal Gevrey class. Adv. Math. , 440:Paper No. 109517, 69, 2024
2024
-
[68]
Wang and L
W. Wang and L. Zhang. The C α regularity of weak solutions of ultraparabolic equations. Discrete Contin. Dyn. Syst. , 29(3):1261–1275, 2011
2011
-
[69]
Wang and L
W. Wang and L. Zhang. C α regularity of weak solutions of non-homogeneous ultrapara bolic equations with drift terms. Sci. China Math. , 67(1):23–44, 2024
2024
-
[70]
Wang and Z
Y. Wang and Z. Zhang. Global C ∞ regularity of the steady Prandtl equation with favorable pr essure gradient. Ann. Inst. H. Poincar´ e C Anal. Non Lin´ eaire, 38(6):1989–2004, 2021
1989
-
[71]
Wang and Z
Y. Wang and Z. Zhang. Asymptotic behavior of the steady P randtl equation. Math. Ann. , 387(3-4):1289– 1331, 2023
2023
-
[72]
D. Wei. Diffusion and mixing in fluid flow via the resolvent estimate. Sci. China Math. , 64(3):507–518, 2021
2021
-
[73]
H. Whitney. Analytic extensions of differentiable func tions defined in closed sets. Transactions of the Amer- ican Mathematical Society , 36(1):63–89, 1934
1934
-
[74]
Xin and L
Z. Xin and L. Zhang. On the global existence of solutions to the Prandtl’s system. Adv. Math. , 181(1):88– 133, 2004
2004
-
[75]
Z. Xin, L. Zhang, and J. Zhao. Global well-posedness and regularity of weak solutions to the Prandtl’s system. SIAM J. Math. Anal. , 56(3):3042–3081, 2024
2024
-
[76]
Xu and X
C. Xu and X. Zhang. Long time well-posedness of Prandtl e quations in Sobolev space. J. Differential Equations, 263(12):8749–8803, 2017
2017
-
[77]
L. Zhang. The C α regularity of a class of ultraparabolic equations. arXiv pr eprint arXiv:math/0510405, 2005
Pith/arXiv arXiv 2005
-
[78]
L. Zhang. The C α regularity of a class of ultraparabolic equations. In Third International Congress of Chinese Mathematicians. Part 1, 2 , volume 42 of AMS/IP Stud. Adv. Math. , pages 619–622. Amer. Math. Soc., Providence, RI, 2008
2008
-
[79]
Zhang and Z
P. Zhang and Z. Zhang. Long time well-posedness of Prand tl system with small and analytic initial data. J. Funct. Anal. , 270(7):2591–2615, 2016. School of Mathematics, University of Minnesota, Minneapol is, Minnesota 55455, USA Email address : jia@umn.edu School of Mathematical Sciences; LMNS and Shanghai Key Labo ratory for Contemporary Applied Mathema...
2016
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