The open questions left by Golse, Lions, Perthame and Sentis (GLPS) in their 1988 paper 'Regularity of the moments of the solution of a transport equation' concern the velocity averaging lemma: if uu solves the stationary transport equation u+v⋅∇xu=fu + v \cdot \nabla_x u = f on RxN×RvN\mathbb{R}^N_x \times \mathbb{R}^N_v and the velocity variable is averaged against a measure μ\mu satisfying a power-law nondegeneracy condition, then the moment u~(x)=∫u(x,v) ϕ(v) dμ(v)\tilde u(x) = \int u(x,v)\,\phi(v)\,d\mu(v) gains fractional regularity in xx. GLPS proved the gain s<γmin⁡(1/p,1/p′)s < \gamma \min(1/p, 1/p') in the Sobolev space Ws,pW^{s,p} (with γ\gamma the nondegeneracy exponent of μ\mu, p′p' the conjugate exponent) and raised the natural sharpness questions. The time-dependent (evolution) variant is absorbed into the modern theory; the sharp exponents are known for the Lebesgue measure (γ=1\gamma = 1) in all LpL^p, 1<p<∞1 < p < \infty; and the p=1p = 1 endpoint fails in general, with a substantial but incomplete substitute theory. What remains open is the general-measure core: necessary and sufficient conditions on μ\mu for a given Sobolev gain, the endpoint characterization at p=1p = 1 and p=∞p = \infty, and the classification of compactness versus failure regimes.

Background

The subject is the regularity in the position variable xx of velocity averages (also called moments) of solutions of linear transport equations. A moment of a phase-space function u(x,v)u(x, v) is the weighted velocity integral u~(x)=∫RNu(x,v) ϕ(v) dμ(v)\tilde u(x) = \int_{\mathbb{R}^N} u(x, v)\,\phi(v)\,d\mu(v), where μ\mu is a positive bounded measure on velocity space and ϕ\phi is a test weight. A velocity averaging lemma asserts that if uu solves a transport equation, in the sense of distributions, with source ff, then u~\tilde u is smoother than a generic function of xx alone: averaging in vv restores a fraction of an xx-derivative. Here smoothness is measured in the Sobolev space Ws,pW^{s,p} (functions with ss fractional derivatives in LpL^p) or the Besov space Bp,rsB^s_{p,r} (a finer scale, obtained by real interpolation, that refines Ws,p=Bp,psW^{s,p} = B^s_{p,p}; roughly Bp,∞sB^s_{p,\infty} contains functions whose smoothness holds at a weak, modulus-of-continuity level). The fundamental result is due to Golse, Lions, Perthame and Sentis (1988), with a compactness precursor by Golse-Perthame-Sentis (1985) and an independent discovery by Agoshkov (1984) in transport theory. GLPS consider the stationary equation u+v⋅∇xu=fu + v \cdot \nabla_x u = f on RxN×RvN\mathbb{R}^N_x \times \mathbb{R}^N_v with u,f∈Lpu, f \in L^p of the phase space (with respect to the product measure dx dμ(v)dx\,d\mu(v)) and μ\mu satisfying the power-law nondegeneracy condition (their (2.1)): sup⁡e∈SN−1μ{v:∣v⋅e∣≤ε}≤Cεγ\sup_{e \in S^{N-1}} \mu\{v : |v \cdot e| \le \varepsilon\} \le C\varepsilon^{\gamma} for all ε>0\varepsilon > 0, where SN−1S^{N-1} is the unit sphere of RN\mathbb{R}^N, with 0<γ<20 < \gamma < 2; this says that no hyperplane through the origin carries too much of the measure, with a power-law rate. Their Theorem 1 gives the Hilbertian gain L2→Hγ/2L^2 \to H^{\gamma/2} (where Hs=Ws,2H^s = W^{s,2}) together with a dyadic-interpolation inequality, and their Theorem 2 gives Lp→Ws,pL^p \to W^{s,p} for s<γmin⁡(1/p,1/p′)s < \gamma \min(1/p, 1/p'), 1<p<∞1 < p < \infty, p′=p/(p−1)p' = p/(p-1). They complement the positive theory with: an L1L^1 compactness criterion for families of moments under uniform integrability (every moment lying below a fixed convex superlinear function, the de la Vallée-Poussin condition); extensions to bounded convex spatial domains with inflow boundary traces (the part of the boundary where the velocity field points inward); Marcinkiewicz weak-LrL^r estimates (bounds in the weak space of functions gg for which tr ∣{∣g∣>t}∣t^r\,|\{|g|>t\}| stays bounded as tt varies) in mixed spaces; a Hölder gain C0,γC^{0,\gamma} in dimension N=1N = 1; and counterexamples, notably an L1L^1 example (Example 1, p. 123) showing that L1L^1 moments of L1L^1 solutions can concentrate on rays and need not gain any Sobolev regularity, plus a kernel family for which equicontinuity fails under L∞L^\infty bounds. Velocity averaging lemmas became a basic tool wherever kinetic equations feed macroscopic limits: the hydrodynamic limits of the Boltzmann equation, the DiPerna-Lions weak solutions of Vlasov-Maxwell, kinetic formulations of scalar conservation laws, and dispersion estimates for Schrödinger-type equations; a 2025 survey by Golse, Mauser and Möller covers the classical, quantum and semi-classical variants. The literature that grew out of GLPS developed along several lines: DiPerna-Lions-Meyer and Bézard extended to LpL^p and Besov scales; Lions and DeVore-Petrova settled the sharp exponents for the Lebesgue measure; Golse-Saint-Raymond, Arsénio-Masmoudi and Arsénio-Lerner built the L1L^1 and duality theory; Jabin-Vega developed real-space methods based on the X-ray transform (the operator integrating a function of position over straight lines, which is the geometry along which the transport equation propagates information); Arsénio and Saint-Raymond connected averaging to hypoellipticity (the phenomenon that solutions of certain degenerate equations are smooth wherever their data are smooth) and compactness; and Erceg, Karlsen and Mitrović reduced the hypotheses on the measure to minimal nondegeneracy assumptions. Terms used below: a velocity measure is the measure μ\mu over which the velocity averaging is performed; a compactness regime is a set of hypotheses on a family of solutions under which the family of moments is relatively compact (equicontinuous after normalization) in a function space on xx alone; an endpoint is the case p=1p = 1 or p=∞p = \infty of an LpL^p scale.

Problem Statement

Let μ\mu be a positive bounded measure on RvN\mathbb{R}^N_v satisfying the GLPS power-law nondegeneracy condition sup⁡e∈SN−1μ{v:∣v⋅e∣≤ε}≤Cεγ\sup_{e \in S^{N-1}} \mu\{v : |v \cdot e| \le \varepsilon\} \le C\varepsilon^{\gamma} for all ε>0\varepsilon > 0 and some 0<γ<20 < \gamma < 2, and let ϕ\phi be a smooth compactly supported velocity weight. For solutions u∈Lp(RxN×RvN; dx dμ(v))u \in L^p(\mathbb{R}^N_x \times \mathbb{R}^N_v;\,dx\,d\mu(v)) (in the sense of distributions) of the stationary transport equation u+v⋅∇xu=fu + v \cdot \nabla_x u = f with source f∈Lp(RxN×RvN; dx dμ(v))f \in L^p(\mathbb{R}^N_x \times \mathbb{R}^N_v;\,dx\,d\mu(v)), the moment u~(x)=∫u(x,v) ϕ(v) dμ(v)\tilde u(x) = \int u(x, v)\,\phi(v)\,d\mu(v) belongs to the Sobolev space Ws,p(RxN)W^{s,p}(\mathbb{R}^N_x) for every s<γmin⁡(1/p,1/p′)s < \gamma\min(1/p, 1/p'), 1<p<∞1 < p < \infty (GLPS Theorem 2). The surviving open core of the questions raised in the source paper is: (i) Sharpness for general measures: determine necessary and sufficient conditions on the measure μ\mu for the moment to lie in Ws,pW^{s,p}. This part requires both of: (a) the sharp gain that holds uniformly over all measures satisfying the power-law nondegeneracy condition with exponent γ\gamma — in particular, whether the bound s<γmin⁡(1/p,1/p′)s < \gamma\min(1/p, 1/p') is the best possible such uniform gain, that is, the worst case over the class — and (b) whether the fine geometry of a fixed measure μ\mu can force a gain strictly larger than that uniform bound, together with what geometric property of μ\mu governs the maximal exponent (the nondegeneracy condition is only an upper bound on the concentration of μ\mu, so a single measure may satisfy it with several exponents γ\gamma, as the Lebesgue case and the mixed-integrability theory illustrate). (ii) Endpoints: characterize the behavior at p=1p = 1, where the naive conclusion fails by the known ray-concentration counterexample, by identifying the exact substitute space (weak-type, Besov B1,∞sB^{s}_{1,\infty}, or otherwise) for moments of L1L^1 solutions; and characterize the p=∞p = \infty endpoint, for which no result is known. (iii) Compactness classification: for families of solutions bounded in Lp(RxN×RvN; dx dμ(v))L^p(\mathbb{R}^N_x \times \mathbb{R}^N_v;\,dx\,d\mu(v)) together with their sources, classify the regimes in which the corresponding family of moments is relatively compact (equicontinuous) in the natural function space on xx alone — relative compactness in Lp(RxN)L^p(\mathbb{R}^N_x), weak relative compactness at the endpoint p=1p = 1, and strong compactness in the Sobolev space Ws,p(RxN)W^{s,p}(\mathbb{R}^N_x) furnished by the averaging estimate with s<γmin⁡(1/p,1/p′)s < \gamma\min(1/p, 1/p') — versus the regimes in which concentration or oscillation destroys compactness, completing the counterexample program of the source paper. Each of (i)-(iii) is an independent open problem: a complete answer to any one of them resolves that corresponding part of the open core, and the open core as a whole is addressed only when all three parts are answered. The time-dependent variant, the Lebesgue-measure sharpness for 1<p<∞1 < p < \infty, and the failure of the naive p=1p = 1 conclusion are settled in the literature and are not part of the open core; no other restriction is imposed on NN, μ\mu, ϕ\phi, or the integrability class.

References

  1. V. I. Agoshkov, 'Spaces of functions with differential-difference characteristics and smoothness of solutions of the transport equation', Sov. Math., Dokl. 29 (1984) 662-666 (translation of Dokl. Akad. Nauk SSSR 276(6) (1984) 1289-1293). zbMATH: https://zbmath.org/?q=an:3966810 (independent discovery of averaging regularity)
  2. F. Golse, B. Perthame, R. Sentis, 'Un résultat de compacité pour les équations de transport et application au calcul de la limite de la valeur propre principale d'un opérateur de transport', C. R. Acad. Sci. Paris Sér. I Math. 301(7) (1985) 341-344. zbMATH: https://zbmath.org/?q=an:3948984 (compactness precursor)
  3. F. Golse, P.-L. Lions, B. Perthame, R. Sentis, 'Regularity of the moments of the solution of a Transport Equation', J. Funct. Anal. 76(1) (1988) 110-125. https://doi.org/10.1016/0022-1236(88)90051-1 (the source paper)
  4. R. J. DiPerna, P.-L. Lions, 'Global weak solutions of Vlasov-Maxwell systems', Comm. Pure Appl. Math. 42(6) (1989) 729-757. https://doi.org/10.1002/cpa.3160420603 (weighted extension of the GLPS averaging used for Vlasov-type systems)
  5. R. J. DiPerna, P.-L. Lions, Y. Meyer, 'LpL^p regularity of velocity averages', Ann. Inst. H. Poincaré Anal. Non Linéaire 8(3) (1991) 271-287. https://doi.org/10.1016/S0294-1449(16)30264-5 (first general non-Hilbertian results, Besov-scale, covering the time-dependent equation)
  6. P. Gérard, 'Moyennisation et régularité deux-microlocale', Ann. Sci. École Norm. Sup. (4) 23(1) (1990) 89-121. https://doi.org/10.24033/asens.1599 (second-microlocal refinement of averaging regularity)
  7. P. Gérard, F. Golse, 'Averaging regularity results for PDEs under transversality assumptions', Comm. Pure Appl. Math. 45(1) (1992) 1-26. https://doi.org/10.1002/cpa.3160450102 (transversality generalization)
  8. M. Bézard, 'Régularité LpL^p précisée des moyennes dans les équations de transport', Bull. Soc. Math. France 122(1) (1994) 29-76. https://doi.org/10.24033/bsmf.2222 (the author states his results are not optimal; the non-homogeneous cases were later found flawed, as reported by Westdickenberg and Arsénio-Masmoudi)
  9. P.-L. Lions, 'Régularité optimale des moyennes en vitesses', C. R. Acad. Sci. Paris Sér. I Math. 320(8) (1995) 911-915. zbMATH: https://zbmath.org/?q=an:772350 (sharpness of the regularity exponents of GLPS and DiPerna-Lions-Meyer for 1≤p≤21 \le p \le 2 via elementary families of examples; published in French with an abridged English version)
  10. R. A. DeVore, G. Petrova, 'The averaging lemma', J. Amer. Math. Soc. 14(2) (2001) 279-296. https://doi.org/10.1090/S0894-0347-00-00359-3 (wavelet counterexamples; Theorem 1.3 shows s≤1/ps \le 1/p necessary for p>2p > 2 in n≥2n \ge 2)
  11. M. Westdickenberg, 'Some new velocity averaging results', SIAM J. Math. Anal. 33(5) (2002) 1007-1032. https://doi.org/10.1137/S0036141000380760 (first mixed-integrability results; identified flaws in the non-homogeneous cases of Bézard 1994)
  12. F. Golse, L. Saint-Raymond, 'Velocity averaging in L1L^1 for the transport equation', C. R. Math. Acad. Sci. Paris 334(7) (2002) 557-562. https://doi.org/10.1016/S1631-073X(02)02302-6 (L1L^1 substitute theory)
  13. P.-E. Jabin, B. Perthame, 'Regularity in kinetic formulations via averaging lemmas', ESAIM Control Optim. Calc. Var. 8 (2002) 761-774. https://doi.org/10.1051/cocv:2002033 (the kinetic-formulation averaging result whose optimality De Lellis-Westdickenberg proved)
  14. C. De Lellis, M. Westdickenberg, 'On the optimality of velocity averaging lemmas', Ann. Inst. H. Poincaré Anal. Non Linéaire 20(6) (2003) 1075-1085. https://doi.org/10.1016/S0294-1449(03)00024-6 (sharpness of the exponents of Jabin-Perthame via Burgers entropy solutions)
  15. P.-E. Jabin, L. Vega, 'Averaging lemmas and the X-ray transform', C. R. Math. Acad. Sci. Paris 337(8) (2003) 505-510. https://doi.org/10.1016/j.crma.2003.09.004 (real-space method)
  16. P.-E. Jabin, L. Vega, 'A real space method for averaging lemmas', J. Math. Pures Appl. (9) 83(11) (2004) 1309-1351. https://doi.org/10.1016/j.matpur.2004.03.004
  17. D. Arsénio, L. Saint-Raymond, 'Compactness in kinetic transport equations and hypoellipticity', J. Funct. Anal. 261(10) (2011) 3044-3098. https://doi.org/10.1016/j.jfa.2011.07.020
  18. D. Arsénio, N. Masmoudi, 'A new approach to velocity averaging lemmas in Besov spaces', J. Math. Pures Appl. (9) 101(4) (2014) 495-551. https://doi.org/10.1016/j.matpur.2013.06.012 (arXiv:1206.6659)
  19. D. Arsénio, 'Recent progress in velocity averaging', Journées équations aux dérivées partielles (2015), Exposé no. 1, 17 p. https://doi.org/10.5802/jedp.630 (https://www.numdam.org/item/JEDP_2015____A1_0/; contains the optimality history and the open Conjectures 9.1-9.3)
  20. D. Arsénio, N. Masmoudi, 'Maximal gain of regularity in velocity averaging lemmas', Anal. PDE 12(2) (2019) 333-388. https://doi.org/10.2140/apde.2019.12.333
  21. D. Arsénio, N. Lerner, 'An energy method for averaging lemmas', Pure Appl. Anal. 3(2) (2021) 319-362. https://doi.org/10.2140/paa.2021.3.319 (arXiv:2006.16058; duality principle and dual-space extensions; records that many questions remain open)
  22. I.-K. Chen, P.-H. Chuang, C.-H. Hsia, J.-K. Su, 'A Revisit of the Velocity Averaging Lemma: on the Regularity of Stationary Boltzmann Equation in a Bounded Convex Domain', arXiv:2011.00180 (2020). https://arxiv.org/abs/2011.00180 (bounded-domain application with fractional Sobolev gains up to order 1−1^-)
  23. T. Erceg, K. H. Karlsen, D. Mitrović, 'Velocity averaging under minimal conditions for deterministic and stochastic kinetic equations with irregular drift', arXiv:2311.01234 (2023). https://arxiv.org/abs/2311.01234 (develops averaging under minimal conditions on the drift using H-distributions)
  24. T. Erceg, K. H. Karlsen, D. Mitrović, 'Regularity of velocity averages in kinetic equations with heterogeneity', arXiv:2507.04102 (2025). https://arxiv.org/abs/2507.04102 (regularity of velocity averages for equations with xx-dependent drift under a quantitative non-degeneracy condition)
  25. F. Golse, N. J. Mauser, J. Möller, 'Velocity Averaging Lemmas: Classical, Quantum and Semi-Classical' (survey), arXiv:2512.01529 (2025). https://arxiv.org/abs/2512.01529 (reaffirms the L1L^1 failure citing GLPS Example 1, p. 123)