v2010.10.26 - Convex Optimization
v2010.10.26 - Convex Optimization v2010.10.26 - Convex Optimization
478 CHAPTER 5. EUCLIDEAN DISTANCE MATRIXD(X) = D(X[0 √ 2V N ]) = D(Q p [0 √ ΛQ T ]) = D([0 √ ΛQ T ]) (1134)This suggests a way to find EDM D given −V T N DV N (confer (1013))[0D =δ ( −VN TDV )N] [1 T + 1 0 δ ( ) ] [−VNDV T T 0 0TN − 20 −VN TDV N](1009)5.12.2 0 geometric center. VAlternatively we may perform reconstruction using auxiliary matrix V(B.4.1) and Gram matrix −V DV 1 (912) instead; to find a generating list2for polyhedronP − α c (1135)whose geometric center has been translated to the origin. Redimensioningdiagonalization factors Q, Λ∈R N×N and unknown Q p ∈ R n×N , (1036)−V DV = 2V X T XV Q √ ΛQ T pQ p√ΛQ T QΛQ T (1136)where the geometrically centered generating list constitutes (confer (1132))XV = 1 √2Q p√ΛQ T ∈ R n×N= [x 1 − 1 N X1 x 2 − 1 N X1 x 3 − 1 N X1 · · · x N − 1 N X1 ] (1137)where α c = 1 N X1. (5.5.1.0.1) The simplest choice for Q p is [ I 0 ]∈ R r×N .Now EDM D can be uniquely made from the list found: (891)D(X) = D(XV ) = D( 1 √2Q p√ΛQ T ) = D( √ ΛQ T ) 1 2(1138)This EDM is, of course, identical to (1134). Similarly to (1009), from −V DVwe can find EDM D (confer (1000))D = δ(−V DV 1 2 )1T + 1δ(−V DV 1 2 )T − 2(−V DV 1 2 ) (999)
5.12. LIST RECONSTRUCTION 479(a)(c)(b)(d)(f)(e)Figure 134: Map of United States of America showing some state boundariesand the Great Lakes. All plots made by connecting 5020 points. Anydifference in scale in (a) through (d) is artifact of plotting routine.(a) Shows original map made from decimated (latitude, longitude) data.(b) Original map data rotated (freehand) to highlight curvature of Earth.(c) Map isometrically reconstructed from an EDM (from distance only).(d) Same reconstructed map illustrating curvature.(e)(f) Two views of one isotonic reconstruction (from comparative distance);problem (1147) with no sort constraint Πd (and no hidden line removal).
- Page 427 and 428: 5.4. EDM DEFINITION 427by translate
- Page 429 and 430: 5.4. EDM DEFINITION 429Crippen & Ha
- Page 431 and 432: 5.4. EDM DEFINITION 431where ([√t
- Page 433 and 434: 5.4. EDM DEFINITION 433because (A.3
- Page 435 and 436: 5.5. INVARIANCE 4355.5.1.0.1 Exampl
- Page 437 and 438: 5.5. INVARIANCE 437x 2 x 2x 3 x 1 x
- Page 439 and 440: 5.6. INJECTIVITY OF D & UNIQUE RECO
- Page 441 and 442: 5.6. INJECTIVITY OF D & UNIQUE RECO
- Page 443 and 444: 5.6. INJECTIVITY OF D & UNIQUE RECO
- Page 445 and 446: 5.7. EMBEDDING IN AFFINE HULL 4455.
- Page 447 and 448: 5.7. EMBEDDING IN AFFINE HULL 447Fo
- Page 449 and 450: 5.7. EMBEDDING IN AFFINE HULL 4495.
- Page 451 and 452: 5.8. EUCLIDEAN METRIC VERSUS MATRIX
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- Page 459 and 460: 5.9. BRIDGE: CONVEX POLYHEDRA TO ED
- Page 461 and 462: 5.9. BRIDGE: CONVEX POLYHEDRA TO ED
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- Page 465 and 466: 5.10. EDM-ENTRY COMPOSITION 465of a
- Page 467 and 468: 5.10. EDM-ENTRY COMPOSITION 467Then
- Page 469 and 470: 5.11. EDM INDEFINITENESS 4695.11.1
- Page 471 and 472: 5.11. EDM INDEFINITENESS 471we have
- Page 473 and 474: 5.11. EDM INDEFINITENESS 473So beca
- Page 475 and 476: 5.11. EDM INDEFINITENESS 475holds o
- Page 477: 5.12. LIST RECONSTRUCTION 477where
- Page 481 and 482: 5.13. RECONSTRUCTION EXAMPLES 481Wi
- Page 483 and 484: 5.13. RECONSTRUCTION EXAMPLES 483d
- Page 485 and 486: 5.13. RECONSTRUCTION EXAMPLES 485Th
- Page 487 and 488: 5.14. FIFTH PROPERTY OF EUCLIDEAN M
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- Page 497 and 498: Chapter 6Cone of distance matricesF
- Page 499 and 500: 6.1. DEFINING EDM CONE 4996.1 Defin
- Page 501 and 502: 6.2. POLYHEDRAL BOUNDS 501This cone
- Page 503 and 504: 6.4. EDM DEFINITION IN 11 T 503That
- Page 505 and 506: 6.4. EDM DEFINITION IN 11 T 505N(1
- Page 507 and 508: 6.4. EDM DEFINITION IN 11 T 507Then
- Page 509 and 510: 6.4. EDM DEFINITION IN 11 T 5096.4.
- Page 511 and 512: 6.5. CORRESPONDENCE TO PSD CONE S N
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- Page 515 and 516: 6.5. CORRESPONDENCE TO PSD CONE S N
- Page 517 and 518: 6.6. VECTORIZATION & PROJECTION INT
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- Page 521 and 522: 6.6. VECTORIZATION & PROJECTION INT
- Page 523 and 524: 6.7. A GEOMETRY OF COMPLETION 523(b
- Page 525 and 526: 6.7. A GEOMETRY OF COMPLETION 525[3
- Page 527 and 528: 6.7. A GEOMETRY OF COMPLETION 527wh
478 CHAPTER 5. EUCLIDEAN DISTANCE MATRIXD(X) = D(X[0 √ 2V N ]) = D(Q p [0 √ ΛQ T ]) = D([0 √ ΛQ T ]) (1134)This suggests a way to find EDM D given −V T N DV N (confer (1013))[0D =δ ( −VN TDV )N] [1 T + 1 0 δ ( ) ] [−VNDV T T 0 0TN − 20 −VN TDV N](1009)5.12.2 0 geometric center. VAlternatively we may perform reconstruction using auxiliary matrix V(B.4.1) and Gram matrix −V DV 1 (912) instead; to find a generating list2for polyhedronP − α c (1135)whose geometric center has been translated to the origin. Redimensioningdiagonalization factors Q, Λ∈R N×N and unknown Q p ∈ R n×N , (1036)−V DV = 2V X T XV Q √ ΛQ T pQ p√ΛQ T QΛQ T (1136)where the geometrically centered generating list constitutes (confer (1132))XV = 1 √2Q p√ΛQ T ∈ R n×N= [x 1 − 1 N X1 x 2 − 1 N X1 x 3 − 1 N X1 · · · x N − 1 N X1 ] (1137)where α c = 1 N X1. (5.5.1.0.1) The simplest choice for Q p is [ I 0 ]∈ R r×N .Now EDM D can be uniquely made from the list found: (891)D(X) = D(XV ) = D( 1 √2Q p√ΛQ T ) = D( √ ΛQ T ) 1 2(1138)This EDM is, of course, identical to (1134). Similarly to (1009), from −V DVwe can find EDM D (confer (1000))D = δ(−V DV 1 2 )1T + 1δ(−V DV 1 2 )T − 2(−V DV 1 2 ) (999)