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v2009.01.01 - Convex Optimization

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7.3. THIRD PREVALENT PROBLEM: 531<br />

7.3.3 Constrained affine dimension, Problem 3<br />

When one desires affine dimension diminished further below what can be<br />

achieved via cenv(rank)-minimization as in (1303), spectral projection can be<br />

considered a natural means in light of its successful application to projection<br />

on a rank ρ subset of the positive semidefinite cone in7.1.4.<br />

Yet it is wrong here to zero eigenvalues of −V DV or −V GV or a<br />

variant to reduce affine dimension, because that particular method comes<br />

from projection on a positive semidefinite cone (1241); zeroing those<br />

eigenvalues here in Problem 3 would place an elbow in the projection<br />

path (confer Figure 129) thereby producing a result that is necessarily<br />

suboptimal. Problem 3 is instead a projection on the EDM cone whose<br />

associated spectral cone is considerably different. (5.11.2.3) Proper choice<br />

of spectral cone is demanded by diagonalization of that variable argument to<br />

the objective:<br />

7.3.3.1 Cayley-Menger form<br />

We use Cayley-Menger composition of the Euclidean distance matrix to solve<br />

a problem that is the same as Problem 3 (1286): (5.7.3.0.1)<br />

[ ] [ ]∥ minimize<br />

0 1<br />

T 0 1<br />

T ∥∥∥<br />

2<br />

D<br />

∥ −<br />

1 −D 1 −H<br />

[ ]<br />

F<br />

0 1<br />

T<br />

(1304)<br />

subject to rank<br />

≤ ρ + 2<br />

1 −D<br />

D ∈ EDM N<br />

a projection of H on a generally nonconvex subset (when ρ < N −1) of the<br />

Euclidean distance matrix cone boundary rel∂EDM N ; id est, projection<br />

from the EDM cone interior or exterior on a subset of its relative boundary<br />

(6.6, (1084)).<br />

Rank of an optimal solution is intrinsically bounded above and below;<br />

[ ] 0 1<br />

T<br />

2 ≤ rank<br />

1 −D ⋆ ≤ ρ + 2 ≤ N + 1 (1305)<br />

Our proposed strategy ([ for low-rank ]) solution is projection on that subset<br />

0 1<br />

T<br />

of a spectral cone λ<br />

1 −EDM N (5.11.2.3) corresponding to affine

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