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60
The Quickhull algorithm for convex hulls
 ACM TRANSACTIONS ON MATHEMATICAL SOFTWARE
, 1996
"... The convex hull of a set of points is the smallest convex set that contains the points. This article presents a practical convex hull algorithm that combines the twodimensional Quickhull Algorithm with the generaldimension BeneathBeyond Algorithm. It is similar to the randomized, incremental algo ..."
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Cited by 713 (0 self)
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algorithms for convex hull and Delaunay triangulation. We provide empirical evidence that the algorithm runs faster when the input contains nonextreme points and that it uses less memory. Computational geometry algorithms have traditionally assumed that input sets are well behaved. When an algorithm
Harmonic superpositions of nonextremal pbranes
 Int. J. Mod. Phys
, 1998
"... The plot of allowed p and D values for pbrane solitons in Ddimensional supergravity is the same whether the solitons are extremal or nonextremal. One of the useful tools for relating different points on the plot is vertical dimensional reduction, which is possible if periodic arrays of pbrane so ..."
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Cited by 2 (0 self)
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The plot of allowed p and D values for pbrane solitons in Ddimensional supergravity is the same whether the solitons are extremal or nonextremal. One of the useful tools for relating different points on the plot is vertical dimensional reduction, which is possible if periodic arrays of p
Prepared for submission to JHEP Phases of nonextremal multicentered bound states
"... Abstract: We investigate the phase space of multicentered nearextremal configurations previously studied in arXiv:1108.5821 [1] and arXiv:1110.5641 [2] in the probe limit. We confirm that in general the energetically favored ground state of the multicenter potential, which can be a single or mult ..."
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limit and rectify it. We also demonstrate that static supertubes can exist inside ergoregions where ordinary point particles would be frame dragged.
Entropy Function for Nonextremal D1D5 and D2D6NS5branes
, 705
"... We apply the entropy function formalism to nonextremal D1D5 and D2D6NS5branes whose throat approximation is given by the Schwarzschild black hole in AdS3× S 3 × T 4 and AdS3 × S 2 × S 1 × T 4, respectively. We find the BekensteinHawking entropy and the (α ′ ) 3 R 4 corrections from the value of th ..."
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Cited by 4 (0 self)
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We apply the entropy function formalism to nonextremal D1D5 and D2D6NS5branes whose throat approximation is given by the Schwarzschild black hole in AdS3× S 3 × T 4 and AdS3 × S 2 × S 1 × T 4, respectively. We find the BekensteinHawking entropy and the (α ′ ) 3 R 4 corrections from the value
2000]Primary: 30A78, 46E15; Secondary: 32A36 STRONGLY EXPOSED POINTS IN THE BALL OF THE
, 2002
"... Abstract. We investigate which boundary points in the closed unit ball of the Bergman space A 1 are strongly exposed. This requires study of the Bergman projection and its kernel, the annihilator of Bergman space. We show that all polynomials in the boundary of the unit ball are strongly exposed. 1. ..."
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. Introduction. In Banach space theory one often seeks to determine the geometry of the unit ball of a given Banach space. A common way to distinguish “round” and “flat ” parts of the boundary of the unit ball is through extreme and nonextreme points. Among the extreme points, or “round ” parts of the boundary,
BPS saturated and nonextreme states in abelian KaluzaKlein theory and effective N = 4 supersymmetric string vacua, arXiv:hepth/9508058; M. Cvetic and D. Youm, All the static spherically symmetric black holes of heterotic string on a six torus, Nucl. Ph
 B
, 1996
"... We summarize results for all fourdimensional Bogomol’nyiSommerfieldPrasat (BPS) saturated and nonextreme solutions of the (4+n)dimensional Abelian KaluzaKlein theory. Within effective N = 4 supersymmetric string vacua, parameterized in terms of fields of the heterotic string on a sixtorus, we ..."
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Cited by 17 (2 self)
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with the corresponding set of nonextreme solutions, are regular with nonzero masses. BPS saturated states with the negative charge norms are singular, unaccompanied by nonextreme solutions and become massless at particular points of the moduli space. The role that such massless states may play in the enhancement
The NonBPS Black Hole Attractor Equation
, 2008
"... We study the attractor mechanism for extremal nonBPS black holes with an infinite throat near horizon geometry, developing, as we do so, a physical argument as to why such a mechanism does not exist in nonextremal cases. We present a detailed derivation of the nonsupersymmetric attractor equati ..."
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Cited by 65 (3 self)
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We study the attractor mechanism for extremal nonBPS black holes with an infinite throat near horizon geometry, developing, as we do so, a physical argument as to why such a mechanism does not exist in nonextremal cases. We present a detailed derivation of the nonsupersymmetric attractor
On Threepoint Functions in the AdS4/CFT3 Correspondence
"... We calculate planar, treelevel, nonextremal threepoint functions of operators belonging to the SU(2)×SU(2) sector of ABJM theory. First, we generalize the determinant representation, found by Foda for the threepoint functions of the SU(2) sector ofN = 4 SYM, to the present case and find that, u ..."
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We calculate planar, treelevel, nonextremal threepoint functions of operators belonging to the SU(2)×SU(2) sector of ABJM theory. First, we generalize the determinant representation, found by Foda for the threepoint functions of the SU(2) sector ofN = 4 SYM, to the present case and find that
Tachyon condensation and black strings
 JHEP
, 2005
"... We show that under certain conditions, closed string tachyon condensation produces a topology changing transition from black strings to KaluzaKlein “bubbles of nothing. ” This can occur when the curvature at the horizon is much smaller than the string scale, so the black string is far from the corr ..."
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Cited by 45 (2 self)
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the correspondence point when it would make a transition to an excited fundamental string. This provides a dramatic new endpoint to Hawking evaporation. A similar transition occurs for black pbranes, and can be viewed as a nonextremal version of a geometric transition. Applications to AdS black holes and the AdS
DIRECT AND REVERSE CARLESON MEASURES FOR H (b) SPACES
"... Abstract. In this paper we discuss direct and reverse Carleson measures for the de BrangesRovnyak spaces H (b), mainly when b is a nonextreme point of the unit ball of H ∞. ..."
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Cited by 1 (1 self)
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Abstract. In this paper we discuss direct and reverse Carleson measures for the de BrangesRovnyak spaces H (b), mainly when b is a nonextreme point of the unit ball of H ∞.
Results 1  10
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