Maximum Principles and Geometric Applications
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Theorem 4. Hopf  for linear elliptic equations.
- Rigoli , Salvatori , Vignati : Some Remarks on the Weak Maximum Principle.
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However there are n The geometric maximum principle is a consequence of the strong maximum principle of Alexandro Let M; g be a spacetime. Then the cosmological time functions: M! It now follows that u is of class C 1,1 , see for example [8, Prop 1. Now assume a ij and b are locally of class C 0, of all its argum The following theorem exten Documents: Advanced Search Include Citations. Galloway , Ralph Howard.
Venue: Comm. Pure Appl.
Math Citations: 24 - 14 self. Citation Context Powered by:. Elliptic partial differential equations of second order, Reprint of the edition - Gilbarg, Trudinger - Foundations of differential geometry - Kobayashi, Nomizu - Eigenvalue comparison theorems and its geometric applications - Cheng - Show Context Citation Context A general comparison theorem with applications to volume estimates for submanifolds - Heintze, Karcher - Show Context Citation Context An extension of E.
Foundations of dierential geometry - Kobayashi, Nomizu - The splitting theorem for spacetimes with strong energy condition - Eschenburg - Show Context Citation Context Regularity of Lorentzian Busemann functions - Galloway, Horta - The cosmological time function. Classical Quantum Gravity 15 - Andersson, Galloway, et al. A proof of the splitting conjecture of s.
The cosmological time function, Class. Table of Contents A crash course in Riemannian geometry. Average Review.
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Maximum Principles and Geometric Applications
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