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Payne: Conservation laws for equations of mixed elliptic-hyperbolic and degenerate types (0)

by D Lupo, K R
Venue:Duke Math. J
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VARIATIONAL EQUATIONS ON MIXED RIEMANNIAN-LORENTZIAN METRICS

by Thomas H. Otway , 2008
"... Abstract. A class of elliptic-hyperbolic equations is placed in the context of a geometric variational theory, in which the change of type is viewed as a change in the character of an underlying metric. A fundamental example of a metric which changes in this way is the extended projective disc, whic ..."
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Abstract. A class of elliptic-hyperbolic equations is placed in the context of a geometric variational theory, in which the change of type is viewed as a change in the character of an underlying metric. A fundamental example of a metric which changes in this way is the extended projective disc, which is Riemannian at ordinary points, Lorentzian at ideal points, and singular on the absolute. Harmonic fields on such a metric can be interpreted as the hodograph image of extremal surfaces in Minkowski 3-space. This suggests an approach to generalized Plateau problems in 3-dimensional space-time via Hodge theory on the extended projective disc. Analogous variational problems arise on Riemannian-Lorentzian flow metrics in fiber bundles (twisted nonlinear Hodge equations), and on certain Riemannian-Lorentzian manifolds which occur in relativity and quantum cosmology. The examples surveyed come with natural gauge theories and Hodge dualities. This paper is mainly a review, but some technical extensions are proven. MSC2000: 35M10, 53A10, 83C80 Key words: signature change, projective disc, Minkowski 3-space, equations of mixed type, nonlinear Hodge equations
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...preted formally as associating a conservation law to the secondorder operator Lφ defined by eq. (16) via the method of multipliers: ∫ ∫ ∫ ∫ 0 = Nφ · Lφdrdθ = dψ. (Compare this equation with p. 262 of =-=[69]-=- and eqs. (5), (6) of [80]; see also the equation preceding eq. (7.1) of [29], taking ∂U/∂t = 0 in that equation.) However, this interpretation is only applicable to a sufficiently small coordinate pa...

POSITIVE SOLUTIONS OF ANISOTROPIC YAMABE–TYPE EQUATIONS IN R n

by Roberto Monti, Daniele Morbidelli
"... Abstract. We study entire positive solutions to the partial differential equation in Rn ∆xu + (α + 1) 2 |x | 2α ∆yu = −|x | 2α u n+2 n−2, where x ∈ R 2, y ∈ R n−2, n ≥ 3 and α> 0. We classify positive solutions with second order derivatives satisfying a suitable growth near the set x = 0. 1. ..."
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Abstract. We study entire positive solutions to the partial differential equation in Rn ∆xu + (α + 1) 2 |x | 2α ∆yu = −|x | 2α u n+2 n−2, where x ∈ R 2, y ∈ R n−2, n ≥ 3 and α> 0. We classify positive solutions with second order derivatives satisfying a suitable growth near the set x = 0. 1.
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... R n is the function u ∗ in R n \ {0} given by u ∗ (z) = ‖z‖ (2−n)(α+1) u (I(z)) . (2.1) The Kelvin transform (2.1) was introduced in [MM] in connection with the study of equation (1.3) (but see also =-=[LP]-=- for the case x ∈ R). The Kelvin transform preserves equation (1.1). Proposition 2.1. If u ∈ C 2 (R n ) is a positive solution of (1.1) in R n , then u ∗ ∈ C 2 (R n \ {0}) is a solution of (1.1) in R ...

L² estimates for the eigenfunctions corresponding to real eigenvalues of the Tricomi operator

by Alberto Favaron , 2009
"... ..."
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umbilical surfaces for

by unknown authors , 2009
"... theorem, conformally invariant cones and ..."
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theorem, conformally invariant cones and
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...m the point of view of nonlinear analysis, sharp inequalities and search for symmetries related to the degenerate elliptic operator ∆α := ∆x + (α + 1) 2 |x| 2α ∆y. (1.13) See, for example, the papers =-=[2, 17, 28, 6, 3, 15, 16]-=-, just to quote a few. The conformal inversion Φ in (1.5) is used in [18], in order to construct a Kelvin–type transform for a semilinear equation with critical nonlinearity of the form −∆αu = u r , f...

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