2009
DOI: 10.1016/j.jcp.2009.05.037
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A spectral solver for evolution problems with spatial -topology

Abstract: We introduce a single patch collocation method in order to compute solutions of initial value problems of partial differential equations whose spatial domains are 3-spheres. Besides the main ideas, we discuss issues related to our implementation and analyze numerical test applications. Our main interest lies in cosmological solutions of Einstein's field equations. Motivated by this, we also elaborate on problems of our approach for general tensorial evolution equations when certain symmetries are assumed. We r… Show more

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Cited by 17 publications
(50 citation statements)
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“…The bundle of orthonormal frames over S 2 and spin-weighted spherical harmonics SO(3) is the bundle of oriented orthonormal frames over S 2 with structure group U (1). Given that SO(3) is double covered by SU (2) and that the latter is diffeomorphic to S 3 , the Hopf map π : S 3 → S 2 can be identified with the bundle map. The theoretical details are discussed, for example, in [4].…”
Section: 3mentioning
confidence: 99%
See 1 more Smart Citation
“…The bundle of orthonormal frames over S 2 and spin-weighted spherical harmonics SO(3) is the bundle of oriented orthonormal frames over S 2 with structure group U (1). Given that SO(3) is double covered by SU (2) and that the latter is diffeomorphic to S 3 , the Hopf map π : S 3 → S 2 can be identified with the bundle map. The theoretical details are discussed, for example, in [4].…”
Section: 3mentioning
confidence: 99%
“…As a consequence of this formalism, our code is (pseudo-)spectral in space; time evolutions are performed with the method of lines and standard ODE integrators (see below). We also point the reader to alternative implementations of this and similar formalisms in [2,10,25].…”
Section: Introductionmentioning
confidence: 99%
“…Eventually, one can exploit the use of an appropriated basis functions adapted to the topology of the conformal time slices -see e.g. [8]-and reduce the evolution equations to a coupled system of ordinary differential equations in the time coordinate, which is then solved with spectral methods. The ultimate aim of this strategy is to depart from the linear equations and solve the full non-linear system of Einstein conformal field equations.…”
Section: Discussionmentioning
confidence: 99%
“…The use of spectral methods in relativistic evolutions can be traced back to pioneering work in the mid-1980s [66] (see also [67, 68, 213]). Over the last decade they have gained popularity, with applications in scenarios as diverse as relativistic hydrodynamics [313, 427, 428], characteristic evolutions [43], absorbing and/or constraint-preserving boundary conditions [314, 369, 365, 363], constraint projection [244], late time “tail” behavior of black-hole perturbations [382, 420], cosmological studies [19, 49, 50], extreme-mass-ratio inspirals within perturbation theory and self-forces [112, 162, 111, 425, 114, 113, 123] and, prominently, binary black-hole simulations (see, for example, [384, 329, 71, 381, 132, 288, 402, 131, 90, 289]) and black-hole-neutron-star ones [150, 168]. The method of lines (Section 7.3) is typically used with a small enough timestep so that the time integration error is smaller than the one due to the spatial approximation and spectral convergence is observed.…”
Section: Spatial Approximations: Spectral Methodsmentioning
confidence: 99%