[{"citation":{"bibtex":"@article{Kang_Lee_Winkler_2022, title={Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $}, volume={42}, DOI={<a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>}, number={115201}, journal={Discrete and Continuous Dynamical Systems}, publisher={American Institute of Mathematical Sciences (AIMS)}, author={Kang, Kyungkeun and Lee, Jihoon and Winkler, Michael}, year={2022} }","mla":"Kang, Kyungkeun, et al. “Global Weak Solutions to a Chemotaxis-Navier-Stokes System in $  \\mathbb{R}^3 $.” <i>Discrete and Continuous Dynamical Systems</i>, vol. 42, no. 11, 5201, American Institute of Mathematical Sciences (AIMS), 2022, doi:<a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>.","short":"K. Kang, J. Lee, M. Winkler, Discrete and Continuous Dynamical Systems 42 (2022).","apa":"Kang, K., Lee, J., &#38; Winkler, M. (2022). Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $. <i>Discrete and Continuous Dynamical Systems</i>, <i>42</i>(11), Article 5201. <a href=\"https://doi.org/10.3934/dcds.2022091\">https://doi.org/10.3934/dcds.2022091</a>","ama":"Kang K, Lee J, Winkler M. Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $. <i>Discrete and Continuous Dynamical Systems</i>. 2022;42(11). doi:<a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>","chicago":"Kang, Kyungkeun, Jihoon Lee, and Michael Winkler. “Global Weak Solutions to a Chemotaxis-Navier-Stokes System in $  \\mathbb{R}^3 $.” <i>Discrete and Continuous Dynamical Systems</i> 42, no. 11 (2022). <a href=\"https://doi.org/10.3934/dcds.2022091\">https://doi.org/10.3934/dcds.2022091</a>.","ieee":"K. Kang, J. Lee, and M. Winkler, “Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $,” <i>Discrete and Continuous Dynamical Systems</i>, vol. 42, no. 11, Art. no. 5201, 2022, doi: <a href=\"https://doi.org/10.3934/dcds.2022091\">10.3934/dcds.2022091</a>."},"intvolume":"        42","year":"2022","issue":"11","publication_status":"published","publication_identifier":{"issn":["1078-0947","1553-5231"]},"doi":"10.3934/dcds.2022091","title":"Global weak solutions to a chemotaxis-Navier-Stokes system in $  \\mathbb{R}^3 $","date_created":"2025-12-18T19:22:04Z","author":[{"full_name":"Kang, Kyungkeun","last_name":"Kang","first_name":"Kyungkeun"},{"full_name":"Lee, Jihoon","last_name":"Lee","first_name":"Jihoon"},{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"volume":42,"publisher":"American Institute of Mathematical Sciences (AIMS)","date_updated":"2025-12-18T20:08:21Z","status":"public","abstract":[{"lang":"eng","text":"<jats:p xml:lang=\"fr\">&lt;p style='text-indent:20px;'&gt;The Cauchy problem in &lt;inline-formula&gt;&lt;tex-math id=\"M2\"&gt;\\begin{document}$  \\mathbb{R}^3 $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; for the chemotaxis-Navier–Stokes system&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id=\"FE1\"&gt; \\begin{document}$ \\begin{eqnarray*} \\left\\{ \\begin{array}{l}      n_t + u\\cdot\\nabla n = \\Delta n - \\nabla \\cdot (n\\nabla c), \\\\\tc_t + u\\cdot\\nabla c = \\Delta c - nc, \\\\ \tu_t + (u\\cdot\\nabla) u = \\Delta u + \\nabla P + n\\nabla\\phi, \\qquad \\nabla \\cdot u = 0, \\ \t\\end{array} \\right. \\end{eqnarray*} $\\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt;&lt;p style='text-indent:20px;'&gt;is considered. Under suitable conditions on the initial data &lt;inline-formula&gt;&lt;tex-math id=\"M3\"&gt;\\begin{document}$ (n_0, c_0, u_0) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, with regard to the crucial first component requiring that &lt;inline-formula&gt;&lt;tex-math id=\"M4\"&gt;\\begin{document}$ n_0\\in L^1( \\mathbb{R}^3) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; be nonnegative and such that &lt;inline-formula&gt;&lt;tex-math id=\"M5\"&gt;\\begin{document}$ (n_0+1)\\ln (n_0+1) \\in L^1( \\mathbb{R}^3) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt;, a globally defined weak solution with &lt;inline-formula&gt;&lt;tex-math id=\"M6\"&gt;\\begin{document}$ (n, c, u)|_{t = 0} = (n_0, c_0, u_0) $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; is constructed. Apart from that, assuming that moreover &lt;inline-formula&gt;&lt;tex-math id=\"M7\"&gt;\\begin{document}$ \\int_{ \\mathbb{R}^3} n_0(x) \\ln (1+|x|^2) dx $\\end{document}&lt;/tex-math&gt;&lt;/inline-formula&gt; is finite, it is shown that a weak solution exists which enjoys further regularity features and preserves mass in an appropriate sense.&lt;/p&gt;</jats:p>"}],"type":"journal_article","publication":"Discrete and Continuous Dynamical Systems","language":[{"iso":"eng"}],"article_number":"5201","user_id":"31496","_id":"63293"},{"volume":41,"date_created":"2025-12-18T19:33:59Z","author":[{"first_name":"Youshan","full_name":"Tao, Youshan","last_name":"Tao"},{"id":"31496","full_name":"Winkler, Michael","last_name":"Winkler","first_name":"Michael"}],"publisher":"American Institute of Mathematical Sciences (AIMS)","date_updated":"2025-12-18T20:04:09Z","doi":"10.3934/dcds.2020216","title":"Critical mass for infinite-time blow-up in a haptotaxis system with nonlinear zero-order interaction","issue":"1","publication_identifier":{"issn":["1553-5231"]},"publication_status":"published","page":"439-454","intvolume":"        41","citation":{"short":"Y. Tao, M. Winkler, Discrete &#38;amp; Continuous Dynamical Systems - A 41 (2020) 439–454.","bibtex":"@article{Tao_Winkler_2020, title={Critical mass for infinite-time blow-up in a haptotaxis system with nonlinear zero-order interaction}, volume={41}, DOI={<a href=\"https://doi.org/10.3934/dcds.2020216\">10.3934/dcds.2020216</a>}, number={1}, journal={Discrete &#38;amp; Continuous Dynamical Systems - A}, publisher={American Institute of Mathematical Sciences (AIMS)}, author={Tao, Youshan and Winkler, Michael}, year={2020}, pages={439–454} }","mla":"Tao, Youshan, and Michael Winkler. “Critical Mass for Infinite-Time Blow-up in a Haptotaxis System with Nonlinear Zero-Order Interaction.” <i>Discrete &#38;amp; Continuous Dynamical Systems - A</i>, vol. 41, no. 1, American Institute of Mathematical Sciences (AIMS), 2020, pp. 439–54, doi:<a href=\"https://doi.org/10.3934/dcds.2020216\">10.3934/dcds.2020216</a>.","apa":"Tao, Y., &#38; Winkler, M. (2020). Critical mass for infinite-time blow-up in a haptotaxis system with nonlinear zero-order interaction. <i>Discrete &#38;amp; Continuous Dynamical Systems - A</i>, <i>41</i>(1), 439–454. <a href=\"https://doi.org/10.3934/dcds.2020216\">https://doi.org/10.3934/dcds.2020216</a>","ieee":"Y. Tao and M. Winkler, “Critical mass for infinite-time blow-up in a haptotaxis system with nonlinear zero-order interaction,” <i>Discrete &#38;amp; Continuous Dynamical Systems - A</i>, vol. 41, no. 1, pp. 439–454, 2020, doi: <a href=\"https://doi.org/10.3934/dcds.2020216\">10.3934/dcds.2020216</a>.","chicago":"Tao, Youshan, and Michael Winkler. “Critical Mass for Infinite-Time Blow-up in a Haptotaxis System with Nonlinear Zero-Order Interaction.” <i>Discrete &#38;amp; Continuous Dynamical Systems - A</i> 41, no. 1 (2020): 439–54. <a href=\"https://doi.org/10.3934/dcds.2020216\">https://doi.org/10.3934/dcds.2020216</a>.","ama":"Tao Y, Winkler M. Critical mass for infinite-time blow-up in a haptotaxis system with nonlinear zero-order interaction. <i>Discrete &#38;amp; Continuous Dynamical Systems - A</i>. 2020;41(1):439-454. doi:<a href=\"https://doi.org/10.3934/dcds.2020216\">10.3934/dcds.2020216</a>"},"year":"2020","user_id":"31496","_id":"63320","language":[{"iso":"eng"}],"publication":"Discrete &amp; Continuous Dynamical Systems - A","type":"journal_article","status":"public"}]
