Blow-up in the Parabolic Scalar Curvature Equation

Details Blow-up in the Parabolic Scalar Curvature Equation Blow-up in the Parabolic Scalar Curvature Equation

2007-05-25

arxiv.org/abs/0705.3774v1

Mathematics

Differential Geometry

Scientific paper

The \textit{parabolic scalar curvature equation} is a reaction-diffusion type equation on an $(n-1)$-manifold $\Sigma$, the time variable of which shall be denoted by $r$. Given a function $R$ on $[r_0,r_1)\times\Sigma$ and a family of metrics $\gamma(r)$ on $\Sigma$, when the coefficients of this equation are appropriately defined in terms of $\gamma$ and $R$, positive solutions give metrics of prescribed scalar curvature $R$ on $[r_0,r_1)\times\Sigma$ in the form $g=u^2dr^2+r^2\gamma$. If the area element of $r^2\gamma$ is expanding for increasing $r$, then the equation is, in fact, uniformly parabolic, and the basic existence problem is to take positive initial data at some $r=r_0$ and solve for $u$ on the maximal interval of existence, which above was implicitly assumed to be $I=[r_0,r_1)$; one often hopes that $r_1=\infty$. However, the case of greatest physical interest, $R>0$, often leads to blow up in finite time so that $r_1<\infty$. It is the purpose of the present work to investigate the situation in which the blow-up nonetheless occurs in such a way that $g$ is continuously extendible to $\bar M=[r_0,r_1]\times\Sigma$ as a manifold with totally geodesic outer boundary at $r=r_1$.

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