---
_id: '63242'
abstract:
- lang: eng
  text: "<jats:title>Abstract</jats:title>\r\n                  <jats:p>\r\n                    For\r\n
    \                   <jats:inline-formula>\r\n                      <jats:alternatives>\r\n
    \                       <jats:tex-math>$$p&gt;2$$</jats:tex-math>\r\n                        <mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                          <mml:mrow>\r\n
    \                           <mml:mi>p</mml:mi>\r\n                            <mml:mo>&gt;</mml:mo>\r\n
    \                           <mml:mn>2</mml:mn>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    , the equation\r\n
    \                   <jats:disp-formula>\r\n                      <jats:alternatives>\r\n
    \                       <jats:tex-math>$$\\begin{aligned} u_t = u^p u_{xx}, \\qquad
    x\\in \\mathbb {R}, \\ t\\in \\mathbb {R}, \\end{aligned}$$</jats:tex-math>\r\n
    \                       <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mtable>\r\n
    \                             <mml:mtr>\r\n                                <mml:mtd>\r\n
    \                                 <mml:mrow>\r\n                                    <mml:msub>\r\n
    \                                     <mml:mi>u</mml:mi>\r\n                                      <mml:mi>t</mml:mi>\r\n
    \                                   </mml:msub>\r\n                                    <mml:mo>=</mml:mo>\r\n
    \                                   <mml:msup>\r\n                                      <mml:mi>u</mml:mi>\r\n
    \                                     <mml:mi>p</mml:mi>\r\n                                    </mml:msup>\r\n
    \                                   <mml:msub>\r\n                                      <mml:mi>u</mml:mi>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:mi>xx</mml:mi>\r\n
    \                                     </mml:mrow>\r\n                                    </mml:msub>\r\n
    \                                   <mml:mo>,</mml:mo>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mi>x</mml:mi>\r\n                                    <mml:mo>∈</mml:mo>\r\n
    \                                   <mml:mi>R</mml:mi>\r\n                                    <mml:mo>,</mml:mo>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mi>t</mml:mi>\r\n
    \                                   <mml:mo>∈</mml:mo>\r\n                                    <mml:mi>R</mml:mi>\r\n
    \                                   <mml:mo>,</mml:mo>\r\n                                  </mml:mrow>\r\n
    \                               </mml:mtd>\r\n                              </mml:mtr>\r\n
    \                           </mml:mtable>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:disp-formula>\r\n                    is shown to admit
    positive and spatially increasing smooth solutions on all of\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$\\mathbb
    {R}\\times \\mathbb {R}$$</jats:tex-math>\r\n                        <mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                          <mml:mrow>\r\n
    \                           <mml:mi>R</mml:mi>\r\n                            <mml:mo>×</mml:mo>\r\n
    \                           <mml:mi>R</mml:mi>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    which are precisely
    of the form of an accelerating wave for\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$t&lt;0$$</jats:tex-math>\r\n
    \                       <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mi>t</mml:mi>\r\n
    \                           <mml:mo>&lt;</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n
    \                         </mml:mrow>\r\n                        </mml:math>\r\n
    \                     </jats:alternatives>\r\n                    </jats:inline-formula>\r\n
    \                   , and of a wave slowing down for\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$t&gt;0$$</jats:tex-math>\r\n
    \                       <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mi>t</mml:mi>\r\n
    \                           <mml:mo>&gt;</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n
    \                         </mml:mrow>\r\n                        </mml:math>\r\n
    \                     </jats:alternatives>\r\n                    </jats:inline-formula>\r\n
    \                   . These solutions satisfy\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$u(\\cdot
    ,t)\\rightarrow 0$$</jats:tex-math>\r\n                        <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mi>u</mml:mi>\r\n
    \                           <mml:mo>(</mml:mo>\r\n                            <mml:mo>·</mml:mo>\r\n
    \                           <mml:mo>,</mml:mo>\r\n                            <mml:mi>t</mml:mi>\r\n
    \                           <mml:mo>)</mml:mo>\r\n                            <mml:mo>→</mml:mo>\r\n
    \                           <mml:mn>0</mml:mn>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    in\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$L^\\infty
    _{loc}(\\mathbb {R})$$</jats:tex-math>\r\n                        <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:msubsup>\r\n
    \                             <mml:mi>L</mml:mi>\r\n                              <mml:mrow>\r\n
    \                               <mml:mi>loc</mml:mi>\r\n                              </mml:mrow>\r\n
    \                             <mml:mi>∞</mml:mi>\r\n                            </mml:msubsup>\r\n
    \                           <mml:mrow>\r\n                              <mml:mo>(</mml:mo>\r\n
    \                             <mml:mi>R</mml:mi>\r\n                              <mml:mo>)</mml:mo>\r\n
    \                           </mml:mrow>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    as\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$t\\rightarrow
    + \\infty $$</jats:tex-math>\r\n                        <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mi>t</mml:mi>\r\n
    \                           <mml:mo>→</mml:mo>\r\n                            <mml:mo>+</mml:mo>\r\n
    \                           <mml:mi>∞</mml:mi>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    and as\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$t\\rightarrow
    -\\infty $$</jats:tex-math>\r\n                        <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mi>t</mml:mi>\r\n
    \                           <mml:mo>→</mml:mo>\r\n                            <mml:mo>-</mml:mo>\r\n
    \                           <mml:mi>∞</mml:mi>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    , and exhibit
    a yet apparently undiscovered phenomenon of transient rapid spatial growth, in
    the sense that\r\n                    <jats:disp-formula>\r\n                      <jats:alternatives>\r\n
    \                       <jats:tex-math>$$\\begin{aligned} \\lim _{x\\rightarrow
    +\\infty } x^{-1} u(x,t) \\quad \\text{ exists } \\text{ for } \\text{ all } t&lt;0,
    \\end{aligned}$$</jats:tex-math>\r\n                        <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mtable>\r\n
    \                             <mml:mtr>\r\n                                <mml:mtd>\r\n
    \                                 <mml:mrow>\r\n                                    <mml:munder>\r\n
    \                                     <mml:mo>lim</mml:mo>\r\n                                      <mml:mrow>\r\n
    \                                       <mml:mi>x</mml:mi>\r\n                                        <mml:mo>→</mml:mo>\r\n
    \                                       <mml:mo>+</mml:mo>\r\n                                        <mml:mi>∞</mml:mi>\r\n
    \                                     </mml:mrow>\r\n                                    </mml:munder>\r\n
    \                                   <mml:msup>\r\n                                      <mml:mi>x</mml:mi>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:mo>-</mml:mo>\r\n
    \                                       <mml:mn>1</mml:mn>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:msup>\r\n                                    <mml:mi>u</mml:mi>\r\n
    \                                   <mml:mrow>\r\n                                      <mml:mo>(</mml:mo>\r\n
    \                                     <mml:mi>x</mml:mi>\r\n                                      <mml:mo>,</mml:mo>\r\n
    \                                     <mml:mi>t</mml:mi>\r\n                                      <mml:mo>)</mml:mo>\r\n
    \                                   </mml:mrow>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mtext>exists</mml:mtext>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mtext>for</mml:mtext>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mtext>all</mml:mtext>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mi>t</mml:mi>\r\n
    \                                   <mml:mo>&lt;</mml:mo>\r\n                                    <mml:mn>0</mml:mn>\r\n
    \                                   <mml:mo>,</mml:mo>\r\n                                  </mml:mrow>\r\n
    \                               </mml:mtd>\r\n                              </mml:mtr>\r\n
    \                           </mml:mtable>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:disp-formula>\r\n                    that\r\n                    <jats:disp-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$\\begin{aligned}
    \\lim _{x\\rightarrow +\\infty } x^{-\\frac{2}{p}} u(x,t) \\quad \\text{ exists
    } \\text{ for } \\text{ all } t&gt;0, \\end{aligned}$$</jats:tex-math>\r\n                        <mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                          <mml:mrow>\r\n
    \                           <mml:mtable>\r\n                              <mml:mtr>\r\n
    \                               <mml:mtd>\r\n                                  <mml:mrow>\r\n
    \                                   <mml:munder>\r\n                                      <mml:mo>lim</mml:mo>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:mi>x</mml:mi>\r\n
    \                                       <mml:mo>→</mml:mo>\r\n                                        <mml:mo>+</mml:mo>\r\n
    \                                       <mml:mi>∞</mml:mi>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:munder>\r\n                                    <mml:msup>\r\n
    \                                     <mml:mi>x</mml:mi>\r\n                                      <mml:mrow>\r\n
    \                                       <mml:mo>-</mml:mo>\r\n                                        <mml:mfrac>\r\n
    \                                         <mml:mn>2</mml:mn>\r\n                                          <mml:mi>p</mml:mi>\r\n
    \                                       </mml:mfrac>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:msup>\r\n                                    <mml:mi>u</mml:mi>\r\n
    \                                   <mml:mrow>\r\n                                      <mml:mo>(</mml:mo>\r\n
    \                                     <mml:mi>x</mml:mi>\r\n                                      <mml:mo>,</mml:mo>\r\n
    \                                     <mml:mi>t</mml:mi>\r\n                                      <mml:mo>)</mml:mo>\r\n
    \                                   </mml:mrow>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mtext>exists</mml:mtext>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mtext>for</mml:mtext>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mtext>all</mml:mtext>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mi>t</mml:mi>\r\n
    \                                   <mml:mo>&gt;</mml:mo>\r\n                                    <mml:mn>0</mml:mn>\r\n
    \                                   <mml:mo>,</mml:mo>\r\n                                  </mml:mrow>\r\n
    \                               </mml:mtd>\r\n                              </mml:mtr>\r\n
    \                           </mml:mtable>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:disp-formula>\r\n                    but that\r\n                    <jats:disp-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$\\begin{aligned}
    u(x,0)=K e^{\\alpha x} \\qquad \\text{ for } \\text{ all } x\\in \\mathbb {R}\\end{aligned}$$</jats:tex-math>\r\n
    \                       <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mtable>\r\n
    \                             <mml:mtr>\r\n                                <mml:mtd>\r\n
    \                                 <mml:mrow>\r\n                                    <mml:mi>u</mml:mi>\r\n
    \                                   <mml:mrow>\r\n                                      <mml:mo>(</mml:mo>\r\n
    \                                     <mml:mi>x</mml:mi>\r\n                                      <mml:mo>,</mml:mo>\r\n
    \                                     <mml:mn>0</mml:mn>\r\n                                      <mml:mo>)</mml:mo>\r\n
    \                                   </mml:mrow>\r\n                                    <mml:mo>=</mml:mo>\r\n
    \                                   <mml:mi>K</mml:mi>\r\n                                    <mml:msup>\r\n
    \                                     <mml:mi>e</mml:mi>\r\n                                      <mml:mrow>\r\n
    \                                       <mml:mi>α</mml:mi>\r\n                                        <mml:mi>x</mml:mi>\r\n
    \                                     </mml:mrow>\r\n                                    </mml:msup>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mtext>for</mml:mtext>\r\n                                    <mml:mspace/>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mtext>all</mml:mtext>\r\n
    \                                   <mml:mspace/>\r\n                                    <mml:mi>x</mml:mi>\r\n
    \                                   <mml:mo>∈</mml:mo>\r\n                                    <mml:mi>R</mml:mi>\r\n
    \                                 </mml:mrow>\r\n                                </mml:mtd>\r\n
    \                             </mml:mtr>\r\n                            </mml:mtable>\r\n
    \                         </mml:mrow>\r\n                        </mml:math>\r\n
    \                     </jats:alternatives>\r\n                    </jats:disp-formula>\r\n
    \                   with some\r\n                    <jats:inline-formula>\r\n
    \                     <jats:alternatives>\r\n                        <jats:tex-math>$$K&gt;0$$</jats:tex-math>\r\n
    \                       <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                         <mml:mrow>\r\n                            <mml:mi>K</mml:mi>\r\n
    \                           <mml:mo>&gt;</mml:mo>\r\n                            <mml:mn>0</mml:mn>\r\n
    \                         </mml:mrow>\r\n                        </mml:math>\r\n
    \                     </jats:alternatives>\r\n                    </jats:inline-formula>\r\n
    \                   and\r\n                    <jats:inline-formula>\r\n                      <jats:alternatives>\r\n
    \                       <jats:tex-math>$$\\alpha &gt;0$$</jats:tex-math>\r\n                        <mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                          <mml:mrow>\r\n
    \                           <mml:mi>α</mml:mi>\r\n                            <mml:mo>&gt;</mml:mo>\r\n
    \                           <mml:mn>0</mml:mn>\r\n                          </mml:mrow>\r\n
    \                       </mml:math>\r\n                      </jats:alternatives>\r\n
    \                   </jats:inline-formula>\r\n                    .\r\n                  </jats:p>"
author:
- first_name: Celina
  full_name: Hanfland, Celina
  last_name: Hanfland
- first_name: Michael
  full_name: Winkler, Michael
  id: '31496'
  last_name: Winkler
citation:
  ama: Hanfland C, Winkler M. Exactly wave-type homoclinic orbits and emergence of
    transient exponential growth in a super-fast diffusion equation. <i>Journal of
    Elliptic and Parabolic Equations</i>. 2025;11(3):2041-2063. doi:<a href="https://doi.org/10.1007/s41808-025-00316-9">10.1007/s41808-025-00316-9</a>
  apa: Hanfland, C., &#38; Winkler, M. (2025). Exactly wave-type homoclinic orbits
    and emergence of transient exponential growth in a super-fast diffusion equation.
    <i>Journal of Elliptic and Parabolic Equations</i>, <i>11</i>(3), 2041–2063. <a
    href="https://doi.org/10.1007/s41808-025-00316-9">https://doi.org/10.1007/s41808-025-00316-9</a>
  bibtex: '@article{Hanfland_Winkler_2025, title={Exactly wave-type homoclinic orbits
    and emergence of transient exponential growth in a super-fast diffusion equation},
    volume={11}, DOI={<a href="https://doi.org/10.1007/s41808-025-00316-9">10.1007/s41808-025-00316-9</a>},
    number={3}, journal={Journal of Elliptic and Parabolic Equations}, publisher={Springer
    Science and Business Media LLC}, author={Hanfland, Celina and Winkler, Michael},
    year={2025}, pages={2041–2063} }'
  chicago: 'Hanfland, Celina, and Michael Winkler. “Exactly Wave-Type Homoclinic Orbits
    and Emergence of Transient Exponential Growth in a Super-Fast Diffusion Equation.”
    <i>Journal of Elliptic and Parabolic Equations</i> 11, no. 3 (2025): 2041–63.
    <a href="https://doi.org/10.1007/s41808-025-00316-9">https://doi.org/10.1007/s41808-025-00316-9</a>.'
  ieee: 'C. Hanfland and M. Winkler, “Exactly wave-type homoclinic orbits and emergence
    of transient exponential growth in a super-fast diffusion equation,” <i>Journal
    of Elliptic and Parabolic Equations</i>, vol. 11, no. 3, pp. 2041–2063, 2025,
    doi: <a href="https://doi.org/10.1007/s41808-025-00316-9">10.1007/s41808-025-00316-9</a>.'
  mla: Hanfland, Celina, and Michael Winkler. “Exactly Wave-Type Homoclinic Orbits
    and Emergence of Transient Exponential Growth in a Super-Fast Diffusion Equation.”
    <i>Journal of Elliptic and Parabolic Equations</i>, vol. 11, no. 3, Springer Science
    and Business Media LLC, 2025, pp. 2041–63, doi:<a href="https://doi.org/10.1007/s41808-025-00316-9">10.1007/s41808-025-00316-9</a>.
  short: C. Hanfland, M. Winkler, Journal of Elliptic and Parabolic Equations 11 (2025)
    2041–2063.
date_created: 2025-12-18T18:57:21Z
date_updated: 2025-12-18T20:16:49Z
doi: 10.1007/s41808-025-00316-9
intvolume: '        11'
issue: '3'
language:
- iso: eng
page: 2041-2063
publication: Journal of Elliptic and Parabolic Equations
publication_identifier:
  issn:
  - 2296-9020
  - 2296-9039
publication_status: published
publisher: Springer Science and Business Media LLC
status: public
title: Exactly wave-type homoclinic orbits and emergence of transient exponential
  growth in a super-fast diffusion equation
type: journal_article
user_id: '31496'
volume: 11
year: '2025'
...
---
_id: '53341'
abstract:
- lang: eng
  text: "<jats:title>Abstract</jats:title><jats:p>The Cauchy problem in <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\mathbb
    {R}^n$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mi>R</mml:mi>\r\n
    \                   </mml:mrow>\r\n                    <mml:mi>n</mml:mi>\r\n
    \                 </mml:msup>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    is considered for the Keller–Segel system <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned}
    \\left\\{ \\begin{array}{l}u_t = \\Delta u - \\nabla \\cdot (u\\nabla v), \\\\
    0 = \\Delta v + u, \\end{array} \\right. \\qquad \\qquad (\\star ) \\end{aligned}$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n
    \                   <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n
    \                         <mml:mrow>\r\n                            <mml:mfenced>\r\n
    \                             <mml:mrow>\r\n                                <mml:mtable>\r\n
    \                                 <mml:mtr>\r\n                                    <mml:mtd>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:msub>\r\n
    \                                         <mml:mi>u</mml:mi>\r\n                                          <mml:mi>t</mml:mi>\r\n
    \                                       </mml:msub>\r\n                                        <mml:mo>=</mml:mo>\r\n
    \                                       <mml:mi>Δ</mml:mi>\r\n                                        <mml:mi>u</mml:mi>\r\n
    \                                       <mml:mo>-</mml:mo>\r\n                                        <mml:mi>∇</mml:mi>\r\n
    \                                       <mml:mo>·</mml:mo>\r\n                                        <mml:mrow>\r\n
    \                                         <mml:mo>(</mml:mo>\r\n                                          <mml:mi>u</mml:mi>\r\n
    \                                         <mml:mi>∇</mml:mi>\r\n                                          <mml:mi>v</mml:mi>\r\n
    \                                         <mml:mo>)</mml:mo>\r\n                                        </mml:mrow>\r\n
    \                                       <mml:mo>,</mml:mo>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:mtd>\r\n                                  </mml:mtr>\r\n
    \                                 <mml:mtr>\r\n                                    <mml:mtd>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:mrow
    />\r\n                                        <mml:mn>0</mml:mn>\r\n                                        <mml:mo>=</mml:mo>\r\n
    \                                       <mml:mi>Δ</mml:mi>\r\n                                        <mml:mi>v</mml:mi>\r\n
    \                                       <mml:mo>+</mml:mo>\r\n                                        <mml:mi>u</mml:mi>\r\n
    \                                       <mml:mo>,</mml:mo>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:mtd>\r\n                                  </mml:mtr>\r\n
    \                               </mml:mtable>\r\n                              </mml:mrow>\r\n
    \                           </mml:mfenced>\r\n                            <mml:mspace
    />\r\n                            <mml:mspace />\r\n                            <mml:mrow>\r\n
    \                             <mml:mo>(</mml:mo>\r\n                              <mml:mo>⋆</mml:mo>\r\n
    \                             <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n
    \                         </mml:mrow>\r\n                        </mml:mtd>\r\n
    \                     </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n
    \               </mml:math></jats:alternatives></jats:disp-formula>with a focus
    on a detailed description of behavior in the presence of nonnegative radially
    symmetric initial data <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:msub>\r\n
    \                   <mml:mi>u</mml:mi>\r\n                    <mml:mn>0</mml:mn>\r\n
    \                 </mml:msub>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    with non-integrable behavior at spatial infinity. It is shown that if <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:msub>\r\n
    \                   <mml:mi>u</mml:mi>\r\n                    <mml:mn>0</mml:mn>\r\n
    \                 </mml:msub>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    is continuous and bounded, then (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star
    $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>)
    admits a local-in-time classical solution, whereas if <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0(x)\\rightarrow
    +\\infty $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mrow>\r\n                    <mml:msub>\r\n                      <mml:mi>u</mml:mi>\r\n
    \                     <mml:mn>0</mml:mn>\r\n                    </mml:msub>\r\n
    \                   <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n
    \                     <mml:mi>x</mml:mi>\r\n                      <mml:mo>)</mml:mo>\r\n
    \                   </mml:mrow>\r\n                    <mml:mo>→</mml:mo>\r\n
    \                   <mml:mo>+</mml:mo>\r\n                    <mml:mi>∞</mml:mi>\r\n
    \                 </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    as <jats:inline-formula><jats:alternatives><jats:tex-math>$$|x|\\rightarrow \\infty
    $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mrow>\r\n                    <mml:mo>|</mml:mo>\r\n                    <mml:mi>x</mml:mi>\r\n
    \                   <mml:mo>|</mml:mo>\r\n                    <mml:mo>→</mml:mo>\r\n
    \                   <mml:mi>∞</mml:mi>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>,
    then no such solution can be found. Furthermore, a collection of three sufficient
    criteria for either global existence or global nonexistence indicates that with
    respect to the occurrence of finite-time blow-up, spatial decay properties of
    an explicit singular steady state plays a critical role. In particular, this underlines
    that explosions in (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star
    $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>)
    need not be enforced by initially high concentrations near finite points, but
    can be exclusively due to large tails.</jats:p>"
author:
- first_name: Michael
  full_name: Winkler, Michael
  last_name: Winkler
citation:
  ama: Winkler M. Solutions to the Keller–Segel system with non-integrable behavior
    at spatial infinity. <i>Journal of Elliptic and Parabolic Equations</i>. 2023;9(2):919-959.
    doi:<a href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>
  apa: Winkler, M. (2023). Solutions to the Keller–Segel system with non-integrable
    behavior at spatial infinity. <i>Journal of Elliptic and Parabolic Equations</i>,
    <i>9</i>(2), 919–959. <a href="https://doi.org/10.1007/s41808-023-00230-y">https://doi.org/10.1007/s41808-023-00230-y</a>
  bibtex: '@article{Winkler_2023, title={Solutions to the Keller–Segel system with
    non-integrable behavior at spatial infinity}, volume={9}, DOI={<a href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>},
    number={2}, journal={Journal of Elliptic and Parabolic Equations}, publisher={Springer
    Science and Business Media LLC}, author={Winkler, Michael}, year={2023}, pages={919–959}
    }'
  chicago: 'Winkler, Michael. “Solutions to the Keller–Segel System with Non-Integrable
    Behavior at Spatial Infinity.” <i>Journal of Elliptic and Parabolic Equations</i>
    9, no. 2 (2023): 919–59. <a href="https://doi.org/10.1007/s41808-023-00230-y">https://doi.org/10.1007/s41808-023-00230-y</a>.'
  ieee: 'M. Winkler, “Solutions to the Keller–Segel system with non-integrable behavior
    at spatial infinity,” <i>Journal of Elliptic and Parabolic Equations</i>, vol.
    9, no. 2, pp. 919–959, 2023, doi: <a href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>.'
  mla: Winkler, Michael. “Solutions to the Keller–Segel System with Non-Integrable
    Behavior at Spatial Infinity.” <i>Journal of Elliptic and Parabolic Equations</i>,
    vol. 9, no. 2, Springer Science and Business Media LLC, 2023, pp. 919–59, doi:<a
    href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>.
  short: M. Winkler, Journal of Elliptic and Parabolic Equations 9 (2023) 919–959.
date_created: 2024-04-07T12:52:52Z
date_updated: 2024-04-07T12:52:55Z
doi: 10.1007/s41808-023-00230-y
intvolume: '         9'
issue: '2'
keyword:
- Applied Mathematics
- Numerical Analysis
- Analysis
language:
- iso: eng
page: 919-959
publication: Journal of Elliptic and Parabolic Equations
publication_identifier:
  issn:
  - 2296-9020
  - 2296-9039
publication_status: published
publisher: Springer Science and Business Media LLC
status: public
title: Solutions to the Keller–Segel system with non-integrable behavior at spatial
  infinity
type: journal_article
user_id: '31496'
volume: 9
year: '2023'
...
---
_id: '63287'
abstract:
- lang: eng
  text: "<jats:title>Abstract</jats:title><jats:p>The Cauchy problem in <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\mathbb
    {R}^n$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:msup>\r\n                    <mml:mrow>\r\n                      <mml:mi>R</mml:mi>\r\n
    \                   </mml:mrow>\r\n                    <mml:mi>n</mml:mi>\r\n
    \                 </mml:msup>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    is considered for the Keller–Segel system <jats:disp-formula><jats:alternatives><jats:tex-math>$$\\begin{aligned}
    \\left\\{ \\begin{array}{l}u_t = \\Delta u - \\nabla \\cdot (u\\nabla v), \\\\
    0 = \\Delta v + u, \\end{array} \\right. \\qquad \\qquad (\\star ) \\end{aligned}$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:mrow>\r\n
    \                   <mml:mtable>\r\n                      <mml:mtr>\r\n                        <mml:mtd>\r\n
    \                         <mml:mrow>\r\n                            <mml:mfenced>\r\n
    \                             <mml:mrow>\r\n                                <mml:mtable>\r\n
    \                                 <mml:mtr>\r\n                                    <mml:mtd>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:msub>\r\n
    \                                         <mml:mi>u</mml:mi>\r\n                                          <mml:mi>t</mml:mi>\r\n
    \                                       </mml:msub>\r\n                                        <mml:mo>=</mml:mo>\r\n
    \                                       <mml:mi>Δ</mml:mi>\r\n                                        <mml:mi>u</mml:mi>\r\n
    \                                       <mml:mo>-</mml:mo>\r\n                                        <mml:mi>∇</mml:mi>\r\n
    \                                       <mml:mo>·</mml:mo>\r\n                                        <mml:mrow>\r\n
    \                                         <mml:mo>(</mml:mo>\r\n                                          <mml:mi>u</mml:mi>\r\n
    \                                         <mml:mi>∇</mml:mi>\r\n                                          <mml:mi>v</mml:mi>\r\n
    \                                         <mml:mo>)</mml:mo>\r\n                                        </mml:mrow>\r\n
    \                                       <mml:mo>,</mml:mo>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:mtd>\r\n                                  </mml:mtr>\r\n
    \                                 <mml:mtr>\r\n                                    <mml:mtd>\r\n
    \                                     <mml:mrow>\r\n                                        <mml:mrow/>\r\n
    \                                       <mml:mn>0</mml:mn>\r\n                                        <mml:mo>=</mml:mo>\r\n
    \                                       <mml:mi>Δ</mml:mi>\r\n                                        <mml:mi>v</mml:mi>\r\n
    \                                       <mml:mo>+</mml:mo>\r\n                                        <mml:mi>u</mml:mi>\r\n
    \                                       <mml:mo>,</mml:mo>\r\n                                      </mml:mrow>\r\n
    \                                   </mml:mtd>\r\n                                  </mml:mtr>\r\n
    \                               </mml:mtable>\r\n                              </mml:mrow>\r\n
    \                           </mml:mfenced>\r\n                            <mml:mspace/>\r\n
    \                           <mml:mspace/>\r\n                            <mml:mrow>\r\n
    \                             <mml:mo>(</mml:mo>\r\n                              <mml:mo>⋆</mml:mo>\r\n
    \                             <mml:mo>)</mml:mo>\r\n                            </mml:mrow>\r\n
    \                         </mml:mrow>\r\n                        </mml:mtd>\r\n
    \                     </mml:mtr>\r\n                    </mml:mtable>\r\n                  </mml:mrow>\r\n
    \               </mml:math></jats:alternatives></jats:disp-formula>with a focus
    on a detailed description of behavior in the presence of nonnegative radially
    symmetric initial data <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:msub>\r\n
    \                   <mml:mi>u</mml:mi>\r\n                    <mml:mn>0</mml:mn>\r\n
    \                 </mml:msub>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    with non-integrable behavior at spatial infinity. It is shown that if <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                  <mml:msub>\r\n
    \                   <mml:mi>u</mml:mi>\r\n                    <mml:mn>0</mml:mn>\r\n
    \                 </mml:msub>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    is continuous and bounded, then (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star
    $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>)
    admits a local-in-time classical solution, whereas if <jats:inline-formula><jats:alternatives><jats:tex-math>$$u_0(x)\\rightarrow
    +\\infty $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mrow>\r\n                    <mml:msub>\r\n                      <mml:mi>u</mml:mi>\r\n
    \                     <mml:mn>0</mml:mn>\r\n                    </mml:msub>\r\n
    \                   <mml:mrow>\r\n                      <mml:mo>(</mml:mo>\r\n
    \                     <mml:mi>x</mml:mi>\r\n                      <mml:mo>)</mml:mo>\r\n
    \                   </mml:mrow>\r\n                    <mml:mo>→</mml:mo>\r\n
    \                   <mml:mo>+</mml:mo>\r\n                    <mml:mi>∞</mml:mi>\r\n
    \                 </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>
    as <jats:inline-formula><jats:alternatives><jats:tex-math>$$|x|\\rightarrow \\infty
    $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mrow>\r\n                    <mml:mo>|</mml:mo>\r\n                    <mml:mi>x</mml:mi>\r\n
    \                   <mml:mo>|</mml:mo>\r\n                    <mml:mo>→</mml:mo>\r\n
    \                   <mml:mi>∞</mml:mi>\r\n                  </mml:mrow>\r\n                </mml:math></jats:alternatives></jats:inline-formula>,
    then no such solution can be found. Furthermore, a collection of three sufficient
    criteria for either global existence or global nonexistence indicates that with
    respect to the occurrence of finite-time blow-up, spatial decay properties of
    an explicit singular steady state plays a critical role. In particular, this underlines
    that explosions in (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\\star
    $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \                 <mml:mo>⋆</mml:mo>\r\n                </mml:math></jats:alternatives></jats:inline-formula>)
    need not be enforced by initially high concentrations near finite points, but
    can be exclusively due to large tails.</jats:p>"
author:
- first_name: Michael
  full_name: Winkler, Michael
  id: '31496'
  last_name: Winkler
citation:
  ama: Winkler M. Solutions to the Keller–Segel system with non-integrable behavior
    at spatial infinity. <i>Journal of Elliptic and Parabolic Equations</i>. 2023;9(2):919-959.
    doi:<a href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>
  apa: Winkler, M. (2023). Solutions to the Keller–Segel system with non-integrable
    behavior at spatial infinity. <i>Journal of Elliptic and Parabolic Equations</i>,
    <i>9</i>(2), 919–959. <a href="https://doi.org/10.1007/s41808-023-00230-y">https://doi.org/10.1007/s41808-023-00230-y</a>
  bibtex: '@article{Winkler_2023, title={Solutions to the Keller–Segel system with
    non-integrable behavior at spatial infinity}, volume={9}, DOI={<a href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>},
    number={2}, journal={Journal of Elliptic and Parabolic Equations}, publisher={Springer
    Science and Business Media LLC}, author={Winkler, Michael}, year={2023}, pages={919–959}
    }'
  chicago: 'Winkler, Michael. “Solutions to the Keller–Segel System with Non-Integrable
    Behavior at Spatial Infinity.” <i>Journal of Elliptic and Parabolic Equations</i>
    9, no. 2 (2023): 919–59. <a href="https://doi.org/10.1007/s41808-023-00230-y">https://doi.org/10.1007/s41808-023-00230-y</a>.'
  ieee: 'M. Winkler, “Solutions to the Keller–Segel system with non-integrable behavior
    at spatial infinity,” <i>Journal of Elliptic and Parabolic Equations</i>, vol.
    9, no. 2, pp. 919–959, 2023, doi: <a href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>.'
  mla: Winkler, Michael. “Solutions to the Keller–Segel System with Non-Integrable
    Behavior at Spatial Infinity.” <i>Journal of Elliptic and Parabolic Equations</i>,
    vol. 9, no. 2, Springer Science and Business Media LLC, 2023, pp. 919–59, doi:<a
    href="https://doi.org/10.1007/s41808-023-00230-y">10.1007/s41808-023-00230-y</a>.
  short: M. Winkler, Journal of Elliptic and Parabolic Equations 9 (2023) 919–959.
date_created: 2025-12-18T19:19:13Z
date_updated: 2025-12-18T20:07:25Z
doi: 10.1007/s41808-023-00230-y
intvolume: '         9'
issue: '2'
language:
- iso: eng
page: 919-959
publication: Journal of Elliptic and Parabolic Equations
publication_identifier:
  issn:
  - 2296-9020
  - 2296-9039
publication_status: published
publisher: Springer Science and Business Media LLC
status: public
title: Solutions to the Keller–Segel system with non-integrable behavior at spatial
  infinity
type: journal_article
user_id: '31496'
volume: 9
year: '2023'
...
---
_id: '53539'
abstract:
- lang: eng
  text: "<jats:title>Abstract</jats:title><jats:p>The infinite Brownian loop on a
    Riemannian manifold is the limit in distribution of the Brownian bridge of length
    <jats:italic>T</jats:italic> around a fixed origin when <jats:inline-formula><jats:alternatives><jats:tex-math>$$T
    \\rightarrow +\\infty $$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \               <mml:mrow>\r\n                  <mml:mi>T</mml:mi>\r\n                  <mml:mo>→</mml:mo>\r\n
    \                 <mml:mo>+</mml:mo>\r\n                  <mml:mi>∞</mml:mi>\r\n
    \               </mml:mrow>\r\n              </mml:math></jats:alternatives></jats:inline-formula>.
    The aim of this note is to study its long-time asymptotics on Riemannian symmetric
    spaces <jats:italic>G</jats:italic>/<jats:italic>K</jats:italic> of noncompact
    type and of general rank. This amounts to the behavior of solutions to the heat
    equation subject to the Doob transform induced by the ground spherical function.
    Unlike the standard Brownian motion, we observe in this case phenomena which are
    similar to the Euclidean setting, namely <jats:inline-formula><jats:alternatives><jats:tex-math>$$L^1$$</jats:tex-math><mml:math
    xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n                <mml:msup>\r\n
    \                 <mml:mi>L</mml:mi>\r\n                  <mml:mn>1</mml:mn>\r\n
    \               </mml:msup>\r\n              </mml:math></jats:alternatives></jats:inline-formula>
    asymptotic convergence without requiring bi-<jats:italic>K</jats:italic>-invariance
    for initial data, and strong <jats:inline-formula><jats:alternatives><jats:tex-math>$$L^{\\infty
    }$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\">\r\n
    \               <mml:msup>\r\n                  <mml:mi>L</mml:mi>\r\n                  <mml:mi>∞</mml:mi>\r\n
    \               </mml:msup>\r\n              </mml:math></jats:alternatives></jats:inline-formula>
    convergence.</jats:p>"
author:
- first_name: Efthymia
  full_name: Papageorgiou, Efthymia
  id: '100325'
  last_name: Papageorgiou
citation:
  ama: Papageorgiou E. Asymptotics for the infinite Brownian loop on noncompact symmetric
    spaces. <i>Journal of Elliptic and Parabolic Equations</i>. Published online 2023.
    doi:<a href="https://doi.org/10.1007/s41808-023-00250-8">10.1007/s41808-023-00250-8</a>
  apa: Papageorgiou, E. (2023). Asymptotics for the infinite Brownian loop on noncompact
    symmetric spaces. <i>Journal of Elliptic and Parabolic Equations</i>. <a href="https://doi.org/10.1007/s41808-023-00250-8">https://doi.org/10.1007/s41808-023-00250-8</a>
  bibtex: '@article{Papageorgiou_2023, title={Asymptotics for the infinite Brownian
    loop on noncompact symmetric spaces}, DOI={<a href="https://doi.org/10.1007/s41808-023-00250-8">10.1007/s41808-023-00250-8</a>},
    journal={Journal of Elliptic and Parabolic Equations}, publisher={Springer Science
    and Business Media LLC}, author={Papageorgiou, Efthymia}, year={2023} }'
  chicago: Papageorgiou, Efthymia. “Asymptotics for the Infinite Brownian Loop on
    Noncompact Symmetric Spaces.” <i>Journal of Elliptic and Parabolic Equations</i>,
    2023. <a href="https://doi.org/10.1007/s41808-023-00250-8">https://doi.org/10.1007/s41808-023-00250-8</a>.
  ieee: 'E. Papageorgiou, “Asymptotics for the infinite Brownian loop on noncompact
    symmetric spaces,” <i>Journal of Elliptic and Parabolic Equations</i>, 2023, doi:
    <a href="https://doi.org/10.1007/s41808-023-00250-8">10.1007/s41808-023-00250-8</a>.'
  mla: Papageorgiou, Efthymia. “Asymptotics for the Infinite Brownian Loop on Noncompact
    Symmetric Spaces.” <i>Journal of Elliptic and Parabolic Equations</i>, Springer
    Science and Business Media LLC, 2023, doi:<a href="https://doi.org/10.1007/s41808-023-00250-8">10.1007/s41808-023-00250-8</a>.
  short: E. Papageorgiou, Journal of Elliptic and Parabolic Equations (2023).
date_created: 2024-04-17T13:16:39Z
date_updated: 2026-07-03T12:36:17Z
department:
- _id: '555'
doi: 10.1007/s41808-023-00250-8
keyword:
- Applied Mathematics
- Numerical Analysis
- Analysis
language:
- iso: eng
publication: Journal of Elliptic and Parabolic Equations
publication_identifier:
  issn:
  - 2296-9020
  - 2296-9039
publication_status: published
publisher: Springer Science and Business Media LLC
status: public
title: Asymptotics for the infinite Brownian loop on noncompact symmetric spaces
type: journal_article
user_id: '100325'
year: '2023'
...
