v2010.10.26 - Convex Optimization
v2010.10.26 - Convex Optimization v2010.10.26 - Convex Optimization
130 CHAPTER 2. CONVEX GEOMETRY2.9.2.8 Positive semidefinite cone is generally not circularExtreme angle equation (239) suggests that the positive semidefinite conemight be invariant to rotation about its axis of revolution; id est, a circularcone. We investigate this now:2.9.2.8.1 Definition. Circular cone: 2.47a pointed closed convex cone having hyperspherical sections orthogonal toits axis of revolution about which the cone is invariant to rotation. △A conic section is the intersection of a cone with any hyperplane. In threedimensions, an intersecting plane perpendicular to a circular cone’s axis ofrevolution produces a section bounded by a circle. (Figure 46) A prominentexample of a circular cone in convex analysis is Lorentz cone (178). Wealso find that the positive semidefinite cone and cone of Euclidean distancematrices are circular cones, but only in low dimension.The positive semidefinite cone has axis of revolution that is the ray(base 0) through the identity matrix I . Consider a set of normalized extremedirections of the positive semidefinite cone: for some arbitrary positiveconstant a∈ R +{yy T ∈ S M | ‖y‖ = √ a} ⊂ ∂S M + (242)The distance from each extreme direction to the axis of revolution is radius√R infc ‖yyT − cI‖ F = a1 − 1 M(243)which is the distance from yy T to a M I ; the length of vector yyT − a M I .Because distance R (in a particular dimension) from the axis of revolutionto each and every normalized extreme direction is identical, the extremedirections lie on the boundary of a hypersphere in isometrically isomorphicR M(M+1)/2 . From Example 2.9.2.7.1, the convex hull (excluding vertex atthe origin) of the normalized extreme directions is a conic sectionC conv{yy T | y ∈ R M , y T y = a} = S M + ∩ {A∈ S M | 〈I , A〉 = a} (244)orthogonal to identity matrix I ;〈C − a 〉M I , I = tr(C − a I) = 0 (245)M
2.9. POSITIVE SEMIDEFINITE (PSD) CONE 131yy TaI θ aMRM 11TFigure 47: Illustrated is a section, perpendicular to axis of revolution, ofcircular cone from Figure 46. Radius R is distance from any extremedirection to axis at a I . Vector aM M 11T is an arbitrary reference by whichto measure angle θ .Proof. Although the positive semidefinite cone possesses somecharacteristics of a circular cone, we can show it is not by demonstratingshortage of extreme directions; id est, some extreme directions correspondingto each and every angle of rotation about the axis of revolution arenonexistent: Referring to Figure 47, [380,1-7]cosθ =〈 aM 11T − a M I , yyT − a M I〉a 2 (1 − 1 M ) (246)Solving for vector y we geta(1 + (M −1) cosθ) = (1 T y) 2 (247)which does not have real solution ∀ 0 ≤ θ ≤ 2π in every matrix dimension M .2.47 A circular cone is assumed convex throughout, although not so by other authors. Wealso assume a right circular cone.
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130 CHAPTER 2. CONVEX GEOMETRY2.9.2.8 Positive semidefinite cone is generally not circularExtreme angle equation (239) suggests that the positive semidefinite conemight be invariant to rotation about its axis of revolution; id est, a circularcone. We investigate this now:2.9.2.8.1 Definition. Circular cone: 2.47a pointed closed convex cone having hyperspherical sections orthogonal toits axis of revolution about which the cone is invariant to rotation. △A conic section is the intersection of a cone with any hyperplane. In threedimensions, an intersecting plane perpendicular to a circular cone’s axis ofrevolution produces a section bounded by a circle. (Figure 46) A prominentexample of a circular cone in convex analysis is Lorentz cone (178). Wealso find that the positive semidefinite cone and cone of Euclidean distancematrices are circular cones, but only in low dimension.The positive semidefinite cone has axis of revolution that is the ray(base 0) through the identity matrix I . Consider a set of normalized extremedirections of the positive semidefinite cone: for some arbitrary positiveconstant a∈ R +{yy T ∈ S M | ‖y‖ = √ a} ⊂ ∂S M + (242)The distance from each extreme direction to the axis of revolution is radius√R infc ‖yyT − cI‖ F = a1 − 1 M(243)which is the distance from yy T to a M I ; the length of vector yyT − a M I .Because distance R (in a particular dimension) from the axis of revolutionto each and every normalized extreme direction is identical, the extremedirections lie on the boundary of a hypersphere in isometrically isomorphicR M(M+1)/2 . From Example 2.9.2.7.1, the convex hull (excluding vertex atthe origin) of the normalized extreme directions is a conic sectionC conv{yy T | y ∈ R M , y T y = a} = S M + ∩ {A∈ S M | 〈I , A〉 = a} (244)orthogonal to identity matrix I ;〈C − a 〉M I , I = tr(C − a I) = 0 (245)M