<?xml version="1.0" encoding="UTF-8"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-10-29T23:52:17Z</responseDate><request verb="GetRecord" identifier="oai:bayburt-rdlopen.rawdatalibrary.net:bayburt/11164" metadataPrefix="oai_dc">https://bayburt-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:bayburt-rdlopen.rawdatalibrary.net:bayburt/11164</identifier><datestamp>2026-10-29T19:35:41Z</datestamp><setSpec>openaire</setSpec><setSpec>com_bayburt_10000</setSpec><setSpec>col_bayburt_10001</setSpec><setSpec>com_bayburt_10007</setSpec><setSpec>col_bayburt_10218</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:title>An attraction–repulsion chemotaxis with logistic source involving the exponents depending on the spatial variables</dc:title><dc:creator>Ayazoglu, Rabil</dc:creator><dc:subject>35K20</dc:subject><dc:subject>35K55</dc:subject><dc:subject>35K59</dc:subject><dc:subject>92C17</dc:subject><dc:subject>Attraction–repulsion</dc:subject><dc:subject>Chemotaxis system</dc:subject><dc:subject>Global boundedness</dc:subject><dc:subject>Logistic source involving the exponents depending on the spatial variables</dc:subject><dc:description>We study the quasilinear attraction–repulsion chemotaxis system of parabolic–elliptic type with logistic source involving the exponents depending on the spatial variables: ut=Δu-χ∇·uu+1r-1∇υ+ξ∇·uu+1r-1∇ω+au-bum(x), 0=Δυ-βυ+αu, 0=Δω-δω+γu, where α, β, δ, γ, χ, ξ, b&gt;0, a≥0, r∈R and m:Ω→1,∞ is a measurable function, subject to the homogeneous Neumann boundary conditions in a bounded domain RNN≥1 with smooth boundary. We prove that this system possesses a unique global bounded classical solution, which is an extension of known results, if the repulsion cancels the attraction in the sense that (balance) χα=ξγ with essinfx∈Ωmx&gt;r+N-2+N,1, and if the attraction prevails over the repulsion in the sense that χα&gt;ξγ with essinfx∈Ωmx&gt;maxr+1,1, and if the repulsion prevails over the attraction in the sense that χα&lt;ξγ.</dc:description><dc:publisher>Birkhauser</dc:publisher><dc:date>2025</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/bayburt/11164</dc:identifier><dc:identifier>https://doi.org/10.1007/s00033-024-02394-6</dc:identifier><dc:identifier>0044-2275</dc:identifier><dc:language>en</dc:language><dc:relation>Zeitschrift fur Angewandte Mathematik und Physik</dc:relation><dc:rights>info:eu-repo/semantics/closedAccess</dc:rights><dc:type>info:eu-repo/semantics/article</dc:type><dc:identifier>https://bayburt-rdlopen.rawdatalibrary.net/tr/items/bayburt/11164</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>