The maximum amount of gene flow, \documentclass[12pt]{minimal}
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\begin{document}$$m_{\max }$$\end{document}, admitting an asymptotically stable two-locus polymorphism as a function of \documentclass[12pt]{minimal}
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\begin{document}$$\phi $$\end{document} or \documentclass[12pt]{minimal}
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\begin{document}$$\rho $$\end{document}. In panels a and b, locus \documentclass[12pt]{minimal}
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\begin{document}$$\mathsf{B }$$\end{document} is under stronger selection than locus \documentclass[12pt]{minimal}
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\begin{document}$$\mathsf{A }$$\end{document} in both demes (\documentclass[12pt]{minimal}
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\begin{document}$$\alpha _2=-2\alpha _1=-1$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\beta _1=-\beta _2=2$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\theta =1$$\end{document}). In c and d, different loci are under stronger selection in the two demes (\documentclass[12pt]{minimal}
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\begin{document}$$\alpha _1=-\beta _2=0.4$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\beta _1=-\alpha _2=2$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\theta =3.84$$\end{document}). Panels a and c show \documentclass[12pt]{minimal}
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\begin{document}$$m_{\max }$$\end{document} as a function of \documentclass[12pt]{minimal}
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\begin{document}$$\phi $$\end{document} for complete linkage (\documentclass[12pt]{minimal}
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\begin{document}$$m_{\max }^0$$\end{document}, (4.61)) and under linkage equilibrium (\documentclass[12pt]{minimal}
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\begin{document}$$m_{\max }^\infty $$\end{document}, (4.43)). Panels b and d display \documentclass[12pt]{minimal}
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\begin{document}$$m_{\max }$$\end{document} for the indicated values of \documentclass[12pt]{minimal}
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\begin{document}$$\phi $$\end{document} as a function of \documentclass[12pt]{minimal}
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\begin{document}$$\rho $$\end{document}. Here, \documentclass[12pt]{minimal}
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\begin{document}$$m_{\max }$$\end{document} is obtained by determining numerically the critical migration rate when the stable internal equilibrium hits the boundary. This is done by computing when the leading eigenvalue at the boundary equilibrium is zero and by calculating the coordinates of the fully polymorphic equilibrium in a small neighborhood. In a and b, we have \documentclass[12pt]{minimal}
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\begin{document}$$\tilde{\phi }^\mathsf{AB }=\tfrac{1}{4}$$\end{document} (indicated by the kink in the dashed line in a), \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{M _1}=\tfrac{5}{17}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{A }=\tfrac{1}{3}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{AB }=\tfrac{3}{8}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{B }=\tfrac{1}{2}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{M _4}=\tfrac{5}{8}$$\end{document}. In c and d, we have \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{M _1}=\tfrac{1}{26}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{A }=\tfrac{1}{6}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{AB }=\tfrac{1}{2}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{B }=\tfrac{5}{6}$$\end{document}, \documentclass[12pt]{minimal}
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\begin{document}$$\phi ^\mathsf{M _4}=\tfrac{25}{26}$$\end{document}