Abstract:We study the "hyperboloidal Cauchy problem" for linear and semilinear wave equations on Minkowski space-time, with initial data in weighted Sobolev spaces allowing singular behaviour at the boundary, or with polyhomogeneous initial data. Specifically, we consider nonlinear symmetric hyperbolic systems of a form which includes scalar fields with a λφ p nonlinearity, as well as wave maps, with initial data given on a hyperboloid; several of the results proved apply to general space-times admitting conformal comp… Show more
“…Denote by∇ the torsion free connection on U which defines with the connection entering (14), (15) the difference tensor∇ −∇ = S(b) and denote byL the tensor (11) derived from∇. Comparing with (12), we find that equations (14), (15) can be written∇ẋẋ…”
Section: Conformal Geodesicsmentioning
confidence: 99%
“…The solution is 'rough' at J ′ and it is expected that it admits a polyhomogeneous expansion there ( [60], cf. also [14]). The evolution of data of type (c) has not been studied yet.…”
Section: The Hyperboloidal Initial Value Problemmentioning
confidence: 99%
“…Denote by f a smooth 1-form field. Then, if x(τ ), b(τ ) solve the conformal geodesics equations (14), (15), the pair x(τ ), b(τ ) − f | x(τ ) solves the same equations with ∇ replaced by the connection∇ =∇ + S(f ) and L byL, i.e. x(τ ), in particular its parameter τ , is independent of the Weyl connection in the conformal class which is used to write the equations.…”
Section: Conformal Geodesicsmentioning
confidence: 99%
“…While it may not be applicable any longer in the desired generality, the underlying idea is viable because the conformal field equations may be used to control also solutions with a 'rough' asymptotic behaviour ( [14], [60], cf. also P. T. Chruściel, this volume).…”
“…Denote by∇ the torsion free connection on U which defines with the connection entering (14), (15) the difference tensor∇ −∇ = S(b) and denote byL the tensor (11) derived from∇. Comparing with (12), we find that equations (14), (15) can be written∇ẋẋ…”
Section: Conformal Geodesicsmentioning
confidence: 99%
“…The solution is 'rough' at J ′ and it is expected that it admits a polyhomogeneous expansion there ( [60], cf. also [14]). The evolution of data of type (c) has not been studied yet.…”
Section: The Hyperboloidal Initial Value Problemmentioning
confidence: 99%
“…Denote by f a smooth 1-form field. Then, if x(τ ), b(τ ) solve the conformal geodesics equations (14), (15), the pair x(τ ), b(τ ) − f | x(τ ) solves the same equations with ∇ replaced by the connection∇ =∇ + S(f ) and L byL, i.e. x(τ ), in particular its parameter τ , is independent of the Weyl connection in the conformal class which is used to write the equations.…”
Section: Conformal Geodesicsmentioning
confidence: 99%
“…While it may not be applicable any longer in the desired generality, the underlying idea is viable because the conformal field equations may be used to control also solutions with a 'rough' asymptotic behaviour ( [14], [60], cf. also P. T. Chruściel, this volume).…”
“…Our methods do not apply in odd space-time dimensions, where the situation is rather different in any case, as one generically expects polyhomogeneous expansions with half-integer powers of 1/r, where r is, say, the luminosity distance, compare [11,26,27,30].…”
Abstract. We show that a set of conformally invariant equations derived from the Fefferman-Graham tensor can be used to construct global solutions of vacuum Einstein equations, in all even dimensions. This gives, in particular, a new, simple proof of Friedrich's result on the future hyperboloidal stability of Minkowski spacetime, and extends its validity to even dimensions.
We describe our present understanding of the relations between the behaviour of asymptotically flat Cauchy data for Einstein's vacuum field equations near space-like infinity and the asymptotic behaviour of their evolution in time at null infinity.
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