v2007.09.13 - Convex Optimization
v2007.09.13 - Convex Optimization v2007.09.13 - Convex Optimization
392 CHAPTER 6. EDM CONE(b)(c)dvec rel∂EDM 3(a)∂H0Figure 95: (a) In isometrically isomorphic subspace R 3 , intersection ofEDM 3 with hyperplane ∂H representing one fixed symmetric entry d 23 =κ(both drawn truncated, rounded vertex is artifact of plot). EDMs in thisdimension corresponding to affine dimension 1 comprise relative boundary ofEDM cone (6.6). Since intersection illustrated includes a nontrivial subsetof cone’s relative boundary, then it is apparent there exist infinitely manyEDM completions corresponding to affine dimension 1. In this dimension it isimpossible to represent a unique nonzero completion corresponding to affinedimension 1, for example, using a single hyperplane because any hyperplanesupporting relative boundary at a particular point Γ contains an entire ray{ζΓ | ζ ≥0} belonging to rel∂EDM 3 by Lemma 2.8.0.0.1. (b) d 13 =κ.(c) d 12 =κ.
6.3.√EDM CONE IS NOT CONVEX 393N = 4. Relative-angle inequality (965) together with four Euclidean metricproperties are necessary and sufficient tests for realizability oftetrahedra. (966) Albeit relative angles θ ikj (766) are nonlinearfunctions of the d ij , relative-angle inequality provides a regulartetrahedron in R 3 [sic] (Figure 92) bounding angles θ ikj at vertex x kconsistently with EDM 4 . 6.2Yet were we to employ the procedure outlined in5.14.3 for makinggeneralized triangle inequalities, then we would find all the necessary andsufficient d ij -transformations for generating bounding polyhedra consistentwith EDMs of any higher dimension (N > 3).6.3 √ EDM cone is not convexFor some applications, like the molecular conformation problem (Figure 3)or multidimensional scaling, [68] [265] absolute distance √ d ij is the preferredvariable. Taking square root of the entries in all EDMs D of dimension N ,we get another cone but not a convex cone when N > 3 (Figure 94(b)):[61,4.5.2]√EDM N ∆ = { ◦√ D | D ∈ EDM N } (985)where ◦√ D is defined as in (984). It is a cone simply because any coneis completely constituted by rays emanating from the origin: (2.7) Anygiven ray {ζΓ∈ R N(N−1)/2 | ζ ≥0} remains a ray under entrywise square root:{ √ ζΓ∈ R N(N−1)/2 | ζ ≥0}. Because of how √ EDM N is defined, it is obviousthat (confer5.10)D ∈ EDM N ⇔ ◦√ √D ∈ EDM N (986)Were √ EDM N convex, then given◦ √ D 1 , ◦√ D 2 ∈ √ EDM N we wouldexpect their conic combination ◦√ D 1 + ◦√ D 2 to be a member of √ EDM N .That is easily proven false by counter-example via (986), for then( ◦√ D 1 + ◦√ D 2 ) ◦( ◦√ D 1 + ◦√ D 2 ) would need to be a member of EDM N .Notwithstanding, in7.2.1 we learn how to transform a nonconvexproximity problem in the natural coordinates √ d ij to a convex optimization.6.2 Still, property-4 triangle inequalities (866) corresponding to each principal 3 ×3submatrix of −VN TDV N demand that the corresponding √ d ij belong to a polyhedralcone like that in Figure 94(b).
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- Page 359 and 360: 5.11. EDM INDEFINITENESS 3595.11.1
- Page 361 and 362: 5.11. EDM INDEFINITENESS 361(confer
- Page 363 and 364: 5.11. EDM INDEFINITENESS 363we have
- Page 365 and 366: 5.11. EDM INDEFINITENESS 365For pre
- Page 367 and 368: 5.12. LIST RECONSTRUCTION 367where
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- Page 387 and 388: Chapter 6EDM coneFor N > 3, the con
- Page 389 and 390: 6.1. DEFINING EDM CONE 3896.1 Defin
- Page 391: 6.2. POLYHEDRAL BOUNDS 391This cone
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- Page 419 and 420: 6.8. DUAL EDM CONE 419When the Fins
- Page 421 and 422: 6.8. DUAL EDM CONE 421Proof. First,
- Page 423 and 424: 6.8. DUAL EDM CONE 423EDM 2 = S 2 h
- Page 425 and 426: 6.8. DUAL EDM CONE 425whose veracit
- Page 427 and 428: 6.8. DUAL EDM CONE 4276.8.1.3.1 Exe
- Page 429 and 430: 6.8. DUAL EDM CONE 429has dual affi
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- Page 435 and 436: 6.10. POSTSCRIPT 435When D is an ED
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- Page 441 and 442: 441HS N h0EDM NK = S N h ∩ R N×N
6.3.√EDM CONE IS NOT CONVEX 393N = 4. Relative-angle inequality (965) together with four Euclidean metricproperties are necessary and sufficient tests for realizability oftetrahedra. (966) Albeit relative angles θ ikj (766) are nonlinearfunctions of the d ij , relative-angle inequality provides a regulartetrahedron in R 3 [sic] (Figure 92) bounding angles θ ikj at vertex x kconsistently with EDM 4 . 6.2Yet were we to employ the procedure outlined in5.14.3 for makinggeneralized triangle inequalities, then we would find all the necessary andsufficient d ij -transformations for generating bounding polyhedra consistentwith EDMs of any higher dimension (N > 3).6.3 √ EDM cone is not convexFor some applications, like the molecular conformation problem (Figure 3)or multidimensional scaling, [68] [265] absolute distance √ d ij is the preferredvariable. Taking square root of the entries in all EDMs D of dimension N ,we get another cone but not a convex cone when N > 3 (Figure 94(b)):[61,4.5.2]√EDM N ∆ = { ◦√ D | D ∈ EDM N } (985)where ◦√ D is defined as in (984). It is a cone simply because any coneis completely constituted by rays emanating from the origin: (2.7) Anygiven ray {ζΓ∈ R N(N−1)/2 | ζ ≥0} remains a ray under entrywise square root:{ √ ζΓ∈ R N(N−1)/2 | ζ ≥0}. Because of how √ EDM N is defined, it is obviousthat (confer5.10)D ∈ EDM N ⇔ ◦√ √D ∈ EDM N (986)Were √ EDM N convex, then given◦ √ D 1 , ◦√ D 2 ∈ √ EDM N we wouldexpect their conic combination ◦√ D 1 + ◦√ D 2 to be a member of √ EDM N .That is easily proven false by counter-example via (986), for then( ◦√ D 1 + ◦√ D 2 ) ◦( ◦√ D 1 + ◦√ D 2 ) would need to be a member of EDM N .Notwithstanding, in7.2.1 we learn how to transform a nonconvexproximity problem in the natural coordinates √ d ij to a convex optimization.6.2 Still, property-4 triangle inequalities (866) corresponding to each principal 3 ×3submatrix of −VN TDV N demand that the corresponding √ d ij belong to a polyhedralcone like that in Figure 94(b).