2012
DOI: 10.1093/mnras/sts401
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On de-Sitter geometry in crater statistics

Abstract: The cumulative size-frequency distributions of impact craters on planetary bodies in the solar system appear to approximate a universal inverse square power-law for small crater radii. In this article, we show how this distribution can be understood easily in terms of geometrical statistics, using a de-Sitter geometry of the configuration space of circles on the Euclidean plane and on the unit sphere. The effect of crater overlap is also considered.

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Cited by 2 publications
(7 citation statements)
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“…As already stressed, this geometric method has-quite surprisingly and to the best of our knowledge-not been employed in the general-relativistic initial-value problem and hardly ever in astrophysics and cosmology. The only two notable exceptions we are aware of concern the statistics of craters on planetary bodies [24] and the statistics of cosmological voids [25] 3 . In our paper we will use it to systematically construct initial data for Einstein's field equations applied to lattice cosmology.…”
Section: Lie Sphere Geometry and Apollonian Packingsmentioning
confidence: 99%
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“…As already stressed, this geometric method has-quite surprisingly and to the best of our knowledge-not been employed in the general-relativistic initial-value problem and hardly ever in astrophysics and cosmology. The only two notable exceptions we are aware of concern the statistics of craters on planetary bodies [24] and the statistics of cosmological voids [25] 3 . In our paper we will use it to systematically construct initial data for Einstein's field equations applied to lattice cosmology.…”
Section: Lie Sphere Geometry and Apollonian Packingsmentioning
confidence: 99%
“…In this fashion the set of spherical caps in S n is not only put into bijective correspondence with points in dS n+1 , but is also endowed with the structure of a maximally symmetric P α cos α Lorentzian manifold with metric g dS (n+1) , the geometry of which turns out to be very useful indeed, with many and sometimes surprising applications. For example, in n = 2 and n = 3 dimensions, the volume form induced by this metric has been used for statistical discussions of distributions of planetary craters in [24] and cosmic voids in [25], respectively. In figure 2 we illustrate once more the geometric objects underlying this bijective correspondence between spherical caps of-or oriented hyperspheres in-the Möbius sphere S n and deSitter space dS (n+1) in the case n = 1.…”
Section: Desitter Space As Configuration Space For Spherical Caps or ...mentioning
confidence: 99%
“…We begin by briefly recapitulating the notion of a configuration space of spheres in Euclidean space and its de-Sitter geometry, as discussed in some more detail in Gibbons & Werner (2013); see also Zee (2013), pp. 646-647.…”
Section: De-sitter Configuration Spacementioning
confidence: 99%
“…Therefore, the space of unoriented spheres is in fact given by half of the full de-Sitter quadric, sometimes referred to as de-Sitter space modulo the antipodal map X µ → −X µ . Geometrically, the coordinates X µ of a sphere can be regarded as a form of Lie cycle coordinates for the Laguerre cycle representing the sphere (see, e.g., the appendix of Gibbons & Werner (2013) for more mathematical details). Taking y i = (R, x), 0 i n + 1, as coordinates of the de-Sitter configuration space, its metric g induced by the ambient Minkowski metric in the usual way can be read off from the line element…”
Section: De-sitter Configuration Spacementioning
confidence: 99%
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