2004
DOI: 10.1088/0264-9381/21/3/012
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The fine structure of Gowdy spacetimes

Abstract: Abstract. The approach to the singularity in Gowdy spacetimes consists of velocity term dominated behavior, except at a set of isolated points. At and near these points, spiky features grow. This paper reviews what is known about these spikes.

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Cited by 9 publications
(20 citation statements)
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“…This is because we are always solving the scalar wave equation with potential where disturbances always propagate within the light cone. In the anisotropic regions "spikes" also form, which are places where the fields change on very small spatial scales, and are similar to regions with this property that have been observerd in numerical simulations of singularities in vacuum spacetimes [11]. Despite the presence of the scalar field, the anisotropic regions exhibit dynamical behavior similar to chaotic mixmaster vacuum solutions, where there are a series of relatively quick transitions between longer epochs where the solution can be described by a w = 1 Bianchi type I spacetime.…”
Section: Introductionmentioning
confidence: 68%
“…This is because we are always solving the scalar wave equation with potential where disturbances always propagate within the light cone. In the anisotropic regions "spikes" also form, which are places where the fields change on very small spatial scales, and are similar to regions with this property that have been observerd in numerical simulations of singularities in vacuum spacetimes [11]. Despite the presence of the scalar field, the anisotropic regions exhibit dynamical behavior similar to chaotic mixmaster vacuum solutions, where there are a series of relatively quick transitions between longer epochs where the solution can be described by a w = 1 Bianchi type I spacetime.…”
Section: Introductionmentioning
confidence: 68%
“…The properties of Gowdy spacetimes have extensively been studied in recent years, both theoretically and numerically. We refer the reader to the works by Garfinkle [6], Isenberg [8], Isenberg and Moncrief [9,10] and Rendall [13,14] and Rendall and Weaver [15], and the references cited therein. Further properties of Gowdy spacetimes have been established by Chae and Chrusciel [4] and Chrusciel and Lake [5].…”
Section: Introductionmentioning
confidence: 99%
“…One can in fact follow this transition in the Weyl tensor directly with an additional first order differential equation which is easily extracted from the Newman-Penrose equations expressed in a frame adapted both to the foliation and the Petrov type of the Weyl tensor. This type of Weyl transition in the spatially homogeneous Mixmaster dynamics can be followed approximately using the Bianchi type II approximation to a curvature bounce, leading to a temporally isolated pulse pair in the real and imaginary parts of the speciality index which represents a circuit ("simple loop around the origin") in the complex plane between the two real asymptotic Kasner points on the interval [0, 1] of the real axis (a "complex pulse"), with profiles in time qualitatively similar to the pairs of spatial profiles present in expansionnormalized metric/shear conjugate variable pairs near the spikes recently found explicitly in spatially inhomogeneous Gowdy cosmologies by Lim [17], and numerically or qualitatively by previous authors [18,19,20,21]. In fact the discontinuity in the asymptotic limit of the speciality index towards the singularity is a gauge invariant characterization of the presence of a "permanent true spike" in the example discussed in Appendix C. These particular spikes seem to describe inhomogeneous discontinuities that seem to arise in asymptotic spatially inhomogeneous BKL dynamics in neighboring curves entering a cosmological singularity.…”
Section: Introductionmentioning
confidence: 76%