v2009.01.01 - Convex Optimization
v2009.01.01 - Convex Optimization v2009.01.01 - Convex Optimization
26 CHAPTER 1. OVERVIEW original reconstruction Figure 6: About five thousand points along the borders constituting the United States were used to create an exhaustive matrix of interpoint distance for each and every pair of points in the ordered set (a list); called a Euclidean distance matrix. From that noiseless distance information, it is easy to reconstruct the map exactly via the Schoenberg criterion (817). (5.13.1.0.1, confer Figure 110) Map reconstruction is exact (to within a rigid transformation) given any number of interpoint distances; the greater the number of distances, the greater the detail (just as it is for all conventional map preparation). is derived, and we also show how to determine if a feasible set belongs exclusively to a positive semidefinite cone boundary. A three-dimensional polyhedral analogue for the positive semidefinite cone of 3 ×3 symmetric matrices is introduced. This analogue is a new tool for visualizing coexistence of low- and high-rank optimal solutions in 6 dimensions. We find a minimum-cardinality Boolean solution to an instance of Ax = b : minimize ‖x‖ 0 x subject to Ax = b x i ∈ {0, 1} , i=1... n (614) The sensor-network localization problem is solved in any dimension in this chapter. We introduce the method of convex iteration for constraining rank in the form rankG ≤ ρ and cardinality in the form cardx ≤ k .
27 Figure 7: These bees construct a honeycomb by solving a convex optimization problem. (5.4.2.2.3) The most dense packing of identical spheres about a central sphere in two dimensions is 6. Packed sphere centers describe a regular lattice. The EDM is studied in chapter 5, Euclidean Distance Matrix, its properties and relationship to both positive semidefinite and Gram matrices. We relate the EDM to the four classical properties of the Euclidean metric; thereby, observing existence of an infinity of properties of the Euclidean metric beyond triangle inequality. We proceed by deriving the fifth Euclidean metric property and then explain why furthering this endeavor is inefficient because the ensuing criteria (while describing polyhedra in angle or area, volume, content, and so on ad infinitum) grow linearly in complexity and number with problem size. Reconstruction methods are explained and applied to a map of the United States; e.g., Figure 6. We also generate a distorted but recognizable isotonic map using only comparative distance information (only ordinal distance data). We demonstrate an elegant method for including dihedral (or torsion) angle constraints into a molecular conformation problem. More geometrical problems solvable via EDMs are presented with the best methods for posing them, EDM problems are posed as convex optimizations, and we show how to recover exact relative position given incomplete noiseless interpoint distance information. The set of all Euclidean distance matrices forms a pointed closed convex cone called the EDM cone, EDM N . We offer a new proof of Schoenberg’s seminal characterization of EDMs: { −V T D ∈ EDM N N DV N ≽ 0 ⇔ (817) D ∈ S N h Our proof relies on fundamental geometry; assuming, any EDM must correspond to a list of points contained in some polyhedron (possibly at
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27<br />
Figure 7: These bees construct a honeycomb by solving a convex optimization<br />
problem. (5.4.2.2.3) The most dense packing of identical spheres about a<br />
central sphere in two dimensions is 6. Packed sphere centers describe a<br />
regular lattice.<br />
The EDM is studied in chapter 5, Euclidean Distance Matrix, its<br />
properties and relationship to both positive semidefinite and Gram matrices.<br />
We relate the EDM to the four classical properties of the Euclidean metric;<br />
thereby, observing existence of an infinity of properties of the Euclidean<br />
metric beyond triangle inequality. We proceed by deriving the fifth Euclidean<br />
metric property and then explain why furthering this endeavor is inefficient<br />
because the ensuing criteria (while describing polyhedra in angle or area,<br />
volume, content, and so on ad infinitum) grow linearly in complexity and<br />
number with problem size.<br />
Reconstruction methods are explained and applied to a map of the<br />
United States; e.g., Figure 6. We also generate a distorted but recognizable<br />
isotonic map using only comparative distance information (only ordinal<br />
distance data). We demonstrate an elegant method for including dihedral<br />
(or torsion) angle constraints into a molecular conformation problem. More<br />
geometrical problems solvable via EDMs are presented with the best methods<br />
for posing them, EDM problems are posed as convex optimizations, and<br />
we show how to recover exact relative position given incomplete noiseless<br />
interpoint distance information.<br />
The set of all Euclidean distance matrices forms a pointed closed convex<br />
cone called the EDM cone, EDM N . We offer a new proof of Schoenberg’s<br />
seminal characterization of EDMs:<br />
{<br />
−V<br />
T<br />
D ∈ EDM N<br />
N DV N ≽ 0<br />
⇔<br />
(817)<br />
D ∈ S N h<br />
Our proof relies on fundamental geometry; assuming, any EDM must<br />
correspond to a list of points contained in some polyhedron (possibly at