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arxiv: 2606.20866 · v1 · pith:QJEJTOJMnew · submitted 2026-06-18 · 🧮 math.AP

Determination of the long-time dynamics for the 2D Keller-Segel equation at critical mass

Pith reviewed 2026-06-26 16:09 UTC · model grok-4.3

classification 🧮 math.AP
keywords Keller-Segel equationcritical masslong-time dynamicssoliton resolutionchemotaxisparabolic-ellipticconcentrationlogarithmic scale
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The pith

Solutions to the 2D Keller-Segel equation at critical mass 8π converge to a renormalized stationary state concentrating around the center of mass on a logarithmic time scale.

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

The paper shows that any solution starting from arbitrary initial data of exactly mass 8π with finite second moment exists for all positive times. As time becomes large the solution approaches a rescaled stationary profile centered at the solution's own center of mass, with the concentration occurring on a universal scale set by the logarithm of time. The result requires no symmetry assumptions on the data and supplies explicit rates. A reader would care because the statement finishes the long-time classification for the model across all mass values when radial symmetry is assumed.

Core claim

For arbitrary initial data with critical mass 8π and finite second momentum, all solutions are globally defined and asymptotically converge to a renormalized stationary state of the equation which concentrates around the center of mass of the solution at a universal logarithmic-in-time scale. Explicit convergence rates are provided. In the radial case the result completes the classification of all possible dynamics: subcritical masses yield self-similar expanders, the critical mass produces the logarithmic concentration described above, and supercritical masses produce finite-time blow-up by type-II concentration of a stationary state.

What carries the argument

Soliton resolution followed by control of the stationary state and remainder in new function spaces, together with multi-scale linearized analysis that yields stability and modulation around an approximate solution.

If this is right

  • All such solutions exist globally in time.
  • The solution converges to a rescaled stationary state centered at its center of mass.
  • The concentration proceeds at a universal logarithmic-in-time rate.
  • Explicit rates of convergence hold without symmetry assumptions.
  • In the radial setting the three mass regimes receive a complete dynamical classification.

Where Pith is reading between the lines

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

  • The logarithmic scale identified here separates global existence from finite-time blow-up and could be checked directly in numerical simulations of the equation.
  • The absence of symmetry requirements suggests the same long-time picture may hold for a broader class of aggregation models without radial symmetry.
  • The modulation and multi-scale techniques developed may adapt to other parabolic-elliptic systems that exhibit critical-mass thresholds.

Load-bearing premise

The initial data has finite second momentum.

What would settle it

An explicit initial datum of mass exactly 8π with finite second moment whose solution either blows up in finite time or fails to approach the claimed renormalized stationary profile at the logarithmic scale.

read the original abstract

We consider the parabolic-elliptic Keller-Segel equation in two dimensions on the whole space. We prove that for arbitrary initial data with critical mass $8\pi$ and finite second momentum, all solutions have the same universal behaviour. They are globally defined and, asymptotically for large times, they converge to a renormalized stationary state of the equation which concentrates around the center of mass of the solution at a universal logarithmic-in-time scale. Our result holds for general solutions without symmetry assumptions, and we furthermore provide explicit convergence rates. In the radial case, by combining our result with previous ones (by Blanchet-Dolbeault-Perthame, Mizoguchi, and related works), this achieves a complete classification of the possible dynamics: for subcritical masses solutions converge to a self-similar expander, at the critical mass they concentrate a stationary state in infinite time at the aforementioned universal scale, and for supercritical masses they blow up in finite time by type II concentration of a stationary state at another universal scale. Our proof starts with soliton resolution, then controls the motion of the stationary state and the remainder in new spaces, and devises new techniques for the multi-scale linearized analysis, which eventually enables the stability and modulation analysis around an approximate solution.

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

0 major / 2 minor

Summary. The manuscript proves that solutions to the 2D parabolic-elliptic Keller-Segel equation with critical mass 8π and finite second momentum are globally defined and, for large times, converge to a renormalized stationary state concentrating around the center of mass at a universal logarithmic time scale, with explicit rates. The result holds without symmetry assumptions. In the radial case, combined with prior works, it yields a complete classification of long-time dynamics across subcritical, critical, and supercritical masses.

Significance. If the central theorem holds, the result is significant: it resolves the critical-mass case for general data, supplies the first non-radial convergence statement at this threshold, and completes the radial classification by combining soliton resolution with prior radial results. The introduction of new function spaces for the modulation analysis and the multi-scale linearization technique constitute a technical advance that may extend to other critical aggregation-diffusion models.

minor comments (2)
  1. [Abstract] The abstract states that the proof 'starts with soliton resolution, then controls the motion of the stationary state and the remainder in new spaces'; a brief outline of the precise function spaces chosen for the remainder (e.g., weighted Sobolev norms or modulation parameters) would help readers follow the strategy before the detailed sections.
  2. [Abstract] The claim of 'explicit convergence rates' is stated without indicating the dependence on the initial second moment; adding a short remark on how the rate constants scale with this quantity would clarify the quantitative aspect of the result.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive summary, significance assessment, and recommendation of minor revision. No major comments were provided in the report, so we have no point-by-point responses to address. We are pleased that the central result, its significance for the critical-mass case without symmetry assumptions, and the technical contributions are viewed favorably.

Circularity Check

0 steps flagged

No significant circularity; derivation is a self-contained PDE proof

full rationale

This is a mathematical existence/uniqueness/stability proof for the 2D Keller-Segel equation at critical mass. The central claim (global existence + logarithmic-in-time concentration to a renormalized stationary state for data with mass 8π and finite second moment) is obtained via soliton resolution, modulation in new function spaces, and multi-scale linearization estimates. The finite-second-moment assumption is stated explicitly as a hypothesis rather than derived. The radial classification step cites prior independent works (Blanchet-Dolbeault-Perthame, Mizoguchi et al.) whose results are not shown to reduce to the present paper. No fitted parameters, self-definitional quantities, ansatz smuggling, or load-bearing self-citations appear in the described strategy. The derivation therefore stands on external mathematical estimates and does not reduce to its own inputs by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Only abstract available; no explicit free parameters, ad-hoc axioms, or invented entities are stated. The result rests on standard well-posedness assumptions for the parabolic-elliptic Keller-Segel system.

axioms (1)
  • standard math The parabolic-elliptic Keller-Segel equation is well-posed for initial data with critical mass and finite second momentum.
    Invoked implicitly to guarantee global existence and the subsequent asymptotic analysis.

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Reference graph

Works this paper leans on

92 extracted references · 6 canonical work pages

  1. [1]

    Barker & C

    T. Barker & C. PrangeLocalized Smoothing for the Navier–Stokes Equations and Concentration of Critical Norms Near SingularitiesArchive for Rational Mechanics and Analysis, Volume 236, pages 1487–1541 (2020)

  2. [2]

    Biler,The Cauchy problem and self-similar solutions for a nonlinear parabolic equation, Studia Mathematica, Volume 114, Issue 2 (1995), Pages 181–205

    P. Biler,The Cauchy problem and self-similar solutions for a nonlinear parabolic equation, Studia Mathematica, Volume 114, Issue 2 (1995), Pages 181–205

  3. [3]

    Biler,Local and global solvability of some parabolic systems modelling chemotaxis, Advances in Mathematical Sciences and Applications, Volume 8 (1998), Pages 715–743

    P. Biler,Local and global solvability of some parabolic systems modelling chemotaxis, Advances in Mathematical Sciences and Applications, Volume 8 (1998), Pages 715–743

  4. [4]

    Biler,Singularities of Solutions to Chemotaxis Systems, De Gruyter Series in Mathematics and Life Sciences, Vol

    P. Biler,Singularities of Solutions to Chemotaxis Systems, De Gruyter Series in Mathematics and Life Sciences, Vol. 6, De Gruyter, 2019

  5. [5]

    Biler, G

    P. Biler, G. Karch, P. Lauren¸ cot, T. NadziejaThe8π-problem for radially symmetric solutions of a chemotaxis model in a disc, Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 27, 2006, 133–147

  6. [6]

    Blanchet, V

    A. Blanchet, V. Calvez, J. A. CarrilloConvergence of the mass-transport steepest descent scheme for the subcritical Patlak-Keller-Segel modelSIAM Journal on Numerical Analysis, Vol. 46, Iss. 2 (2008)

  7. [7]

    Blanchet, E

    A. Blanchet, E. Carlen, J. A. CarrilloFunctional inequalities, thick tails and asymptotics for the critical mass Pat- lak–Keller–Segel modelJournal of Functional Analysis Volume 262, Issue 5, 1 March 2012, Pages 2142-2230

  8. [8]

    Blanchet, J

    A. Blanchet, J. A. Carrillo, N. MasmoudiInfinite time aggregation for the critical Patlak-Keller-Segel model inR 2, Communications on Pure and Applied MathematicsVolume 61, Issue 10 pp. 1449-1481

  9. [9]

    Blanchet, J

    A. Blanchet, J. Dolbeault, M. Escobedo and J. Fern´ andez,Asymptotic behaviour for small mass in the two-dimensional parabolic-elliptic Keller–Segel model, Journal of Mathematical Analysis and Applications, Volume 361, Issue 2 (2010), Pages 533–542

  10. [10]

    Blanchet, J

    A. Blanchet, J. Dolbeault, B. PerthameTwo-dimensional Keller-Segel model: optimal critical mass and qualitative properties of the solutionsElectron. J. Differential Equations, (2006), pp. No. 44, 32

  11. [11]

    Brezis & T

    H. Brezis & T. CazenaveA nonlinear heat equation with singular initial dataJ. Anal. Math. 68, 277–304 (1996)

  12. [12]

    Buseghin & C

    F. Buseghin & C. CollotClassification of the dynamics of radial solutions to the 2D parabolic-elliptic Keller-Segel SystemTo appear

  13. [13]

    Buseghin, J

    F. Buseghin, J. D´ avila, M. del Pino, M. Musso,Existence of finite time blow-up in Keller-Segel system, Annals of PDE12(2026), Article 17

  14. [14]

    Caffarelli, R

    L. Caffarelli, R. Kohn, and L. NirenbergPartial regularity of suitable weak solutions of the Navier-Stokes equations Comm. Pure Appl. Math., 35(6):771–831, (1982)

  15. [15]

    J. Campos SerranoMod` eles attractifs en astrophysique et biologie: points critiques et comportement en temps grand des solutionsPhD thesis, Th` ese de l’Universit´ e Paris Dauphine, 2012

  16. [16]

    J. F. Campos & J. DolbeaultA functional framework for the Keller-Segel system: logarithmic Hardy-LittlewoodSobolev and related spectral gap inequalitiesC. R. Math. Acad. Sci. Paris, 350 (2012), pp. 949–954

  17. [17]

    J. F. Campos and J. Dolbeault,Asymptotic Estimates for the Parabolic-Elliptic Keller–Segel Model in the Plane, Communications in Partial Differential Equations, Volume 39, Issue 5 (2014), Pages 806–841

  18. [18]

    E. A. Carlen,Stability for the logarithmic Hardy–Littlewood–Sobolev inequality with application to the Keller–Segel equation, J. Funct. Anal. 288 (2025), no. 6, 111081

  19. [19]

    Carlen & A

    E. Carlen & A. FigalliStability for a GNS inequality and the log-HLS inequality, with application to the critical mass Keller-Segel equationDuke Math. J., 162 (2013), pp. 579–625

  20. [20]

    Carlen & M

    E. Carlen & M. LossCompeting symmetries, the logarithmic HLS inequality and Onofri’s inequality onS n Geom. Funct. Anal., 2 (1992), pp. 90–104

  21. [21]

    Carrillo, S

    J.A. Carrillo, S. Hittmeir, B. Volzone & Y. YaoNonlinear aggregation–diffusion equations: radial symmetry and long time asymptotics, Inventiones mathematicae, Volume 218, pages 889–977 (2019)

  22. [22]

    P. H. Chavanis,Nonlinear mean field Fokker–Planck equations. Application to the chemotaxis of biological populations, The European Physical Journal B, Volume 62 (2008), Pages 179–208

  23. [23]

    P. H. Chavanis & C. SireVirial theorem and dynamical evolution of self-gravitating Brownian particles in an unbounded domain. I. Overdamped models, , Phys. Rev. E (3), 73 (2006), pp. 066103, 16

  24. [24]

    Chen & C

    W. Chen & C. LiClassification of solutions of some nonlinear elliptic equationsDuke Math. J. 63(3): 615-622 (August 1991)

  25. [25]

    Childress and J

    S. Childress and J. K. Percus,Nonlinear aspects of chemotaxis, Mathematical Biosciences, Volume 56, Issues 3–4 (1981), Pages 217–237

  26. [26]

    Collot, T

    C. Collot, T. Duyckaerts, C. Kenig, & F. MerleSoliton resolution and channels of energy.Advanced Nonlinear Studies, 25(2), 279-284 (2025)

  27. [27]

    Collot, T.-E

    C. Collot, T.-E. Ghoul, N. Masmoudi, V. T. NguyenSpectral analysis for singularity formation of the two dimensional Keller-Segel systemAnn. PDE, 8 (2022), pp. Paper No. 5, 74

  28. [28]

    Collot, T.-E

    C. Collot, T.-E. Ghoul, N. Masmoudi, V. T. NguyenRefined Description and Stability for Singular Solutions of the 2D Keller-Segel SystemCommunications on Pure and Applied Mathematics / Volume 75, Issue 7 pp. 1419-1516

  29. [29]

    Collot, T.-E

    C. Collot, T.-E. Ghoul, N. Masmoudi, V. T. NguyenSingularity formed by the collision of two collapsing solitons in interaction for the 2D Keller-Segel systemarXiv:2409.05363

  30. [30]

    Collot, P

    C. Collot, P. Rapha¨ el, J. Szeftel,On the stability of type I blow up for the energy super critical heat equation, Mem. Amer. Math. Soc., 260 (2019), pp. v+97

  31. [31]

    Collot, K

    C. Collot, K. Zhang,On the stability of Type I self-similar blowups for the Keller-Segel system in three dimensions and higher, arXiv:2406.11358v2 (2024)

  32. [32]

    Collot, F

    C. Collot, F. Merle, & P. Rapha¨ el .Dynamics near the ground state for the energy critical nonlinear heat equation in large dimensions.Communications in Mathematical Physics, 352(1), 215-285 (2017)

  33. [33]

    E. B. Davies,Heat Kernels and Spectral Theory, Cambridge University Press, Cambridge, 1989

  34. [34]

    D´ avila, M

    J. D´ avila, M. del Pino, J. Dolbeault, M. Musso, J. WeiExistence and stability of infinite time blow-up in the Keller- Segel system, Arch Rational Mech Anal 248, 61 (2024) LONG-TIME DYNAMICS FOR THE 2D KELLER–SEGEL EQUATION AT CRITICAL MASS 77

  35. [35]

    D` avila, M

    J. D` avila, M. del Pino, & J. Wei .Singularity formation for the two-dimensional harmonic map flow intoS 2. Inven- tiones mathematicae, 219(2), 345-466 (2020)

  36. [36]

    del Pino & J

    M. del Pino & J. DolbeaultBest constants for Gagliardo-Nirenberg inequalities and applications to nonlinear diffusions Jour. Math. Pures Appl., 81: 301–342

  37. [37]

    Dolbeault and C

    J. Dolbeault and C. Schmeiser,The two-dimensional Keller–Segel model after blow-up, Discrete and Continuous Dynamical Systems, Volume 25, Issue 1 (2009), Pages 109–121

  38. [38]

    J. I. Diaz, T. Nagai and J.-M. Rakotoson,Symmetrization Techniques on Unbounded Domains: Application to a Chemotaxis System onR N, Journal of Differential Equations, Volume 145, Issue 1 (1998), Pages 156–183

  39. [39]

    Duyckaerts, H

    T. Duyckaerts, H. Jia, C. Kenig, & F. Merle .Soliton resolution along a sequence of times for the focusing energy critical wave equation. Geometric and Functional Analysis, 27(4), 798-862 (2017)

  40. [40]

    Duyckaerts & F

    T. Duyckaerts & F. MerleDynamic of threshold solutions for energy-critical NLSGeometric and Functional Analysis, 18(6), 1787-1840 (2009)

  41. [41]

    Duyckaerts & F

    T. Duyckaerts & F. MerleDynamics of threshold solutions for energy-critical wave equation.International Mathe- matics Research Papers, 2008, rpn002 (2008)

  42. [42]

    Ega˜ na Fern´ andez & S

    G. Ega˜ na Fern´ andez & S. MischlerUniqueness and long time asymptotic for the Keller-Segel equation: the parabolic- elliptic caseArch. Ration. Mech. Anal., 220 (2016), pp. 1159–1194

  43. [43]

    Elbar, A

    C. Elbar, A. Fern´ andez-Jim´ enez, F. Santambrogio,A Li–Yau and Aronson–B´ enilan approach for the Keller–Segel system with critical exponent, arXiv:2512.17772, (2025)

  44. [44]

    Ghoul & N

    T-E. Ghoul & N. MasmoudiMinimal mass blowup solutions for the Patlak-Keller-Segel equation, Communications on Pure and Applied Mathematics / Volume 71, Issue 10 pp. 1957-2015

  45. [45]

    M. A. Herrero & J. J. L. Vel´ azquezChemotactic collapse for the Keller-Segel modelJ. Math. Biol., 35 (1996), pp. 177–194

  46. [46]

    M. A. Herrero & J. J. L. Vel´ azquezSingularity patterns in a chemotaxis modelMath. Ann., 306 (1996), pp. 583–623

  47. [47]

    M. A. Herrero & J. J. L. Vel´ azquezA blow-up mechanism for a chemotaxis modelAnn. Scuola Norm. Sup. Pisa Cl. Sci. (4), 24 (1997), pp. 633–683 (1998)

  48. [48]

    Hillen and K

    T. Hillen and K. J. Painter,A user’s guide to PDE models for chemotaxis, Journal of Mathematical Biology, Volume 58 (2009), Pages 183–217

  49. [49]

    Horstmann,From 1970 Until Present: the Keller-Segel Model in Chemotaxis and Its Consequences, Nieders¨ achsische Staats- und Universit¨ atsbibliothek, 2003

    D. Horstmann,From 1970 Until Present: the Keller-Segel Model in Chemotaxis and Its Consequences, Nieders¨ achsische Staats- und Universit¨ atsbibliothek, 2003

  50. [50]

    HosonoGlobal existence for the fully parabolic Keller–Segel system with critical mass on the planearXiv preprint arXiv:2602.03768 (2026)

    T. HosonoGlobal existence for the fully parabolic Keller–Segel system with critical mass on the planearXiv preprint arXiv:2602.03768 (2026)

  51. [51]

    Jeong, K

    U. Jeong, K. Kim, T. Kim, & S. Kwon.Classification of single-bubble blow-up solutions for Calogero–Moser derivative nonlinear Schr¨ odinger equation.arXiv preprint arXiv:2601.07410 (2026)

  52. [52]

    K. Kim & F. MerleOn classification of global dynamics for energy-critical equivariant harmonic map heat flows and radial nonlinear heat equation.Communications on Pure and Applied Mathematics, 78(9), 1783-1842 (2025)

  53. [53]

    K. Kim & F. MerleRigidity results in multi-bubble dynamics for non-radial energy-critical heat equationarXiv preprint arXiv:2601.12517 (2026)

  54. [54]

    J¨ ager and S

    W. J¨ ager and S. Luckhaus,On Explosions of Solutions to a System of Partial Differential Equations Modelling Chemotaxis, Transactions of the American Mathematical Society, Volume 329, No. 2 (1992), Pages 819–824

  55. [55]

    Jendrej & A

    J. Jendrej & A. LawrieTwo-bubble dynamics for threshold solutions to the wave maps equationInventiones mathe- maticae, 213(3), 1249-1325 (2018)

  56. [56]

    I., & Souplet, P

    Kavallaris, N. I., & Souplet, P. (2009). Grow-up rate and refined asymptotics for a two-dimensional Patlak–Keller–Segel model in a disk. SIAM journal on mathematical analysis, 40(5), 1852-1881

  57. [57]

    KatoPerturbation Theory for Linear Operators, 2nd ed., Springer-Verlag, Berlin–Heidelberg–New York, 1980

    T. KatoPerturbation Theory for Linear Operators, 2nd ed., Springer-Verlag, Berlin–Heidelberg–New York, 1980

  58. [58]

    E. F. Keller and L. A. Segel,Model for chemotaxis, Journal of Theoretical Biology, Volume 30, Issue 2 (1971), Pages 225–234

  59. [59]

    L´ opez-G´ omez, T

    J. L´ opez-G´ omez, T. Nagai, T. Yamada,Non-trivialω-limit sets and oscillating solutions in a chemotaxis model in R2 with critical mass, J. Funct. Anal., 266 (2014), pp. 3455–3507

  60. [60]

    E. H. Lieb,Sharp constants in the Hardy–Littlewood–Sobolev and related inequalities, Annals of Mathematics, Vol. 118, No. 2 (1983), Pages 349–374

  61. [61]

    G. M. Lieberman,Second Order Parabolic Differential Equations, World Scientific Publishing Co., 1996

  62. [62]

    F. LinA new proof of the Caffarelli-Kohn-Nirenberg theoremCommunications on Pure and Applied Mathematics: A Journal Issued by the Courant Institute of Mathematical Sciences, 51(3):241–257, (1998)

  63. [63]

    L´ opez-G´ omez, T

    J. L´ opez-G´ omez, T. Nagai and T. Yamada,The Basin of Attraction of the Steady-States for a Chemotaxis Model in R2 with Critical Mass, Archive for Rational Mechanics and Analysis, Volume 207 (2013), Pages 159–184

  64. [64]

    L´ opez-G´ omez, T

    J. L´ opez-G´ omez, T. Nagai, T. YamadaNon-trivialω-limit sets and oscillating solutions in a chemotaxis model inR 2 with critical massJ. Funct. Anal., 266 (2014), pp. 3455–3507

  65. [65]

    Matano & F

    H. Matano & F. MerleOn nonexistence of type II blowup for a supercritical nonlinear heat equationCommunications on Pure and Applied Mathematics: A Journal Issued by the Courant Institute of Mathematical Sciences, 57(11), 1494-1541 (2004)

  66. [66]

    Martel, F

    Y. Martel, F. Merle, & P. Rapha¨ elBlow up for the critical gKdV equation. II: Minimal mass dynamicsJournal of the European Mathematical Society (EMS Publishing), 17(8) (2015)

  67. [67]

    MerleDetermination of blow-up solutions with minimal mass for nonlinear Schr¨ odinger equations with critical powerDuke Math

    F. MerleDetermination of blow-up solutions with minimal mass for nonlinear Schr¨ odinger equations with critical powerDuke Math. J. 69(2): 427-454 (1993)

  68. [68]

    MizoguchiRate of type II blowup for a semilinear heat equation

    N. MizoguchiRate of type II blowup for a semilinear heat equation. Mathematische Annalen, 339(4), 839-877 (2007)

  69. [69]

    N. MizoguchiGlobal existence for the cauchy problem of the parabolic–parabolic Keller–Segel system on the plane Calculus of Variations and Partial Differential Equations, 48(3), 491-505 (2013)

  70. [70]

    MizoguchiRefined asymptotic behavior of blowup solutions to a simplified chemotaxis systemComm

    N. MizoguchiRefined asymptotic behavior of blowup solutions to a simplified chemotaxis systemComm. Pure Appl. Math., 75 (2022), pp. 1870–1886. 78 F. BUSEGHIN AND C. COLLOT

  71. [71]

    T. Nagai,Blowup of nonradial solutions to parabolic-elliptic systems modeling chemotaxis in two-dimensional domains, Journal of Inequalities and Applications, Volume 6, Issue 1 (2001), Pages 37–55

  72. [72]

    NagaiConvergence to self-similar solutions for a parabolic-elliptic system of drift-diffusion type inR 2, Adv

    T. NagaiConvergence to self-similar solutions for a parabolic-elliptic system of drift-diffusion type inR 2, Adv. Differential Equations, 16 (2011), pp. 839–866

  73. [73]

    Nagai and T

    T. Nagai and T. Senba,Behavior of radially symmetric solutions of a system related to chemotaxis, Nonlinear Analysis: Theory, Methods & Applications, Volume 30, Issue 6 (1997), Pages 3837–3842

  74. [74]

    Naito, T

    Y. Naito, T. Senba,Bounded and unbounded oscillating solutions to a parabolic-elliptic system in two dimensional space, Commun. Pure Appl. Anal., 12 (2013), pp. 1861–1880

  75. [75]

    Naito, T

    Y. Naito, T. Suzuki,Self-similarity in Chemotaxis Systems, Colloq. Math., 111 (2008), no. 1, pp. 11–34

  76. [76]

    OttoThe geometry of dissipative evolution equations: the porous medium equationCommunications in Partial Differential Equations Volume 26, (2001) - Issue 1-2

    F. OttoThe geometry of dissipative evolution equations: the porous medium equationCommunications in Partial Differential Equations Volume 26, (2001) - Issue 1-2

  77. [77]

    C. S. Patlak,Random walk with persistence and external bias, Bulletin of Mathematical Biology, Volume 15, Pages 311–338

  78. [78]

    Rapha¨ el and R

    P. Rapha¨ el and R. SchweyerOn the stability of critical chemotactic aggregationMath. Ann., 359 (2014), pp. 267–377

  79. [79]

    Rapha¨ el, P., & Szeftel, J. (2011). Existence and uniqueness of minimal blow-up solutions to an inhomogeneous mass critical NLS. Journal of the American Mathematical Society, 24(2), 471-546

  80. [80]

    Y. Seki, Y. Sugiyama, J. J. L. Vel´ azquezMultiple peak aggregations for the Keller–Segel systemNonlinearity 26 319

Showing first 80 references.