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v2009.01.01 - Convex Optimization

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190 CHAPTER 2. CONVEX GEOMETRY<br />

A natural question pertains to whether a theory of unique coordinates,<br />

like biorthogonal expansion, is extensible to proper cones whose extreme<br />

directions number in excess of ambient spatial dimensionality.<br />

2.13.11.0.4 Theorem. Conic coordinates.<br />

With respect to vector v in some finite-dimensional Euclidean space R n ,<br />

define a coordinate t ⋆ v of point x in full-dimensional pointed closed convex<br />

cone K<br />

t ⋆ v(x) ∆ = sup{t∈ R | x − tv ∈ K} (432)<br />

Given points x and y in cone K , if t ⋆ v(x)= t ⋆ v(y) for each and every extreme<br />

direction v of K then x = y .<br />

⋄<br />

2.13.11.0.5 Proof. Vector x −t ⋆ v must belong to the cone<br />

boundary ∂K by definition (432). So there must exist a nonzero vector λ that<br />

is inward-normal to a hyperplane supporting cone K and containing x −t ⋆ v ;<br />

id est, by boundary membership relation for full-dimensional pointed closed<br />

convex cones (2.13.2)<br />

x−t ⋆ v ∈ ∂K ⇔ ∃ λ ≠ 0 〈λ, x−t ⋆ v〉 = 0, λ ∈ K ∗ , x−t ⋆ v ∈ K (298)<br />

where<br />

K ∗ = {w ∈ R n | 〈v , w〉 ≥ 0 for all v ∈ G(K)} (332)<br />

is the full-dimensional pointed closed convex dual cone. The set G(K) , of<br />

possibly infinite cardinality N , comprises generators for cone K ; e.g., its<br />

extreme directions which constitute a minimal generating set. If x −t ⋆ v<br />

is nonzero, any such vector λ must belong to the dual cone boundary by<br />

conjugate boundary membership relation<br />

λ ∈ ∂K ∗ ⇔ ∃ x−t ⋆ v ≠ 0 〈λ, x−t ⋆ v〉 = 0, x−t ⋆ v ∈ K , λ ∈ K ∗ (299)<br />

where<br />

K = {z ∈ R n | 〈λ, z〉 ≥ 0 for all λ ∈ G(K ∗ )} (331)<br />

This description of K means: cone K is an intersection of halfspaces whose<br />

inward-normals are generators of the dual cone. Each and every face of<br />

cone K (except the cone itself) belongs to a hyperplane supporting K . Each<br />

and every vector x −t ⋆ v on the cone boundary must therefore be orthogonal<br />

to an extreme direction constituting generators G(K ∗ ) of the dual cone.

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