Fitting affine and orthogonal transformations between two sets of points

Similar documents
The Symmetric and Antipersymmetric Solutions of the Matrix Equation A 1 X 1 B 1 + A 2 X 2 B A l X l B l = C and Its Optimal Approximation

Product Cosines of Angles between Subspaces

Algorithms to solve massively under-defined systems of multivariate quadratic equations

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries

Combining reaction kinetics to the multi-phase Gibbs energy calculation

MARKOV CHAINS AND MARKOV DECISION THEORY. Contents

Improving the Reliability of a Series-Parallel System Using Modified Weibull Distribution

ORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION

Lecture Note 3: Stationary Iterative Methods

CS229 Lecture notes. Andrew Ng

Componentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems

Wavelet Galerkin Solution for Boundary Value Problems

Multilayer Kerceptron

David Eigen. MA112 Final Paper. May 10, 2002

Math 124B January 17, 2012

BALANCING REGULAR MATRIX PENCILS

DIGITAL FILTER DESIGN OF IIR FILTERS USING REAL VALUED GENETIC ALGORITHM

Gaussian Curvature in a p-orbital, Hydrogen-like Atoms

Partial permutation decoding for MacDonald codes

An Algorithm for Pruning Redundant Modules in Min-Max Modular Network

Separation of Variables and a Spherical Shell with Surface Charge

Lecture 6: Moderately Large Deflection Theory of Beams

A Brief Introduction to Markov Chains and Hidden Markov Models

A proposed nonparametric mixture density estimation using B-spline functions

XSAT of linear CNF formulas

Higher dimensional PDEs and multidimensional eigenvalue problems

(This is a sample cover image for this issue. The actual cover is not yet available at this time.)

FRST Multivariate Statistics. Multivariate Discriminant Analysis (MDA)

Problem set 6 The Perron Frobenius theorem.

A. Distribution of the test statistic

The EM Algorithm applied to determining new limit points of Mahler measures

Haar Decomposition and Reconstruction Algorithms

LECTURE 10. The world of pendula

ASummaryofGaussianProcesses Coryn A.L. Bailer-Jones

Akaike Information Criterion for ANOVA Model with a Simple Order Restriction

Theory of Generalized k-difference Operator and Its Application in Number Theory

Matrices and Determinants

A Solution to the 4-bit Parity Problem with a Single Quaternary Neuron

ON THE REPRESENTATION OF OPERATORS IN BASES OF COMPACTLY SUPPORTED WAVELETS

Interactive Fuzzy Programming for Two-level Nonlinear Integer Programming Problems through Genetic Algorithms

Integrating Factor Methods as Exponential Integrators

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

LECTURE NOTES 9 TRACELESS SYMMETRIC TENSOR APPROACH TO LEGENDRE POLYNOMIALS AND SPHERICAL HARMONICS

4 Separation of Variables

arxiv:nlin/ v2 [nlin.cd] 30 Jan 2006

Alberto Maydeu Olivares Instituto de Empresa Marketing Dept. C/Maria de Molina Madrid Spain

Theory and implementation behind: Universal surface creation - smallest unitcell

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

THINKING IN PYRAMIDS

The distribution of the number of nodes in the relative interior of the typical I-segment in homogeneous planar anisotropic STIT Tessellations

18-660: Numerical Methods for Engineering Design and Optimization

Model Solutions (week 4)

Assignment 7 Due Tuessday, March 29, 2016

c 2007 Society for Industrial and Applied Mathematics

A Two-Parameter Trigonometric Series

Published in: Proceedings of the Twenty Second Nordic Seminar on Computational Mechanics

4 1-D Boundary Value Problems Heat Equation

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z

LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS

TRANSFORMATION OF REAL SPHERICAL HARMONICS UNDER ROTATIONS

BP neural network-based sports performance prediction model applied research

Research Article On the Lower Bound for the Number of Real Roots of a Random Algebraic Equation


Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator

ALGORITHMIC SUMMATION OF RECIPROCALS OF PRODUCTS OF FIBONACCI NUMBERS. F. = I j. ^ = 1 ^ -, and K w = ^. 0) n=l r n «=1 -*/!

Research Article Numerical Range of Two Operators in Semi-Inner Product Spaces

Appendix A: MATLAB commands for neural networks

Two-Stage Least Squares as Minimum Distance

Introduction. Figure 1 W8LC Line Array, box and horn element. Highlighted section modelled.

Smoothness equivalence properties of univariate subdivision schemes and their projection analogues

Introduction to PDEs and Numerical Methods Tutorial 10. Finite Element Analysis

Lecture Notes for Math 251: ODE and PDE. Lecture 32: 10.2 Fourier Series

Introduction to LMTO method

An explicit Jordan Decomposition of Companion matrices

addenda and errata addenda and errata

Data Search Algorithms based on Quantum Walk

CONJUGATE GRADIENT WITH SUBSPACE OPTIMIZATION

Restricted weak type on maximal linear and multilinear integral maps.

1D Heat Propagation Problems

MAT 167: Advanced Linear Algebra

Establishment of Weak Conditions for Darboux- Goursat-Beudon Theorem

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes

Effect of transport ratio on source term in determination of surface emission coefficient

Efficient Generation of Random Bits from Finite State Markov Chains

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES

arxiv: v1 [math.ca] 6 Mar 2017

FRIEZE GROUPS IN R 2

Stochastic Variational Inference with Gradient Linearization

Convolutional Networks 2: Training, deep convolutional networks

Post-buckling behaviour of a slender beam in a circular tube, under axial load

$, (2.1) n="# #. (2.2)

The Group Structure on a Smooth Tropical Cubic

A Novel Learning Method for Elman Neural Network Using Local Search

HYDROGEN ATOM SELECTION RULES TRANSITION RATES

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and

Worst Case Analysis of the Analog Circuits

CS 331: Artificial Intelligence Propositional Logic 2. Review of Last Time

14 Separation of Variables Method

ANALOG OF HEAT EQUATION FOR GAUSSIAN MEASURE OF A BALL IN HILBERT SPACE GYULA PAP

Lecture 9: Submatrices and Some Special Matrices

Transcription:

Mathematica Communications 9(2004), 27-34 27 Fitting affine and orthogona transformations between two sets of points Hemuth Späth Abstract. Let two point sets P and Q be given in R n. We determine a transation and an affine transformation or an isometry such that the image of Q approximates P as best as possibe in the east squares sense. Key words: fitting inear transformations, east squares AMS subject cassifications: 65D10 Received May 28, 2003 Accepted February 20, 2004 1. Introduction Let the two sets of points P and Q by given by p i =(p 1i,...,p ni ) T, q i =(a 1i,...,a ni ) T (i =1,...,m). (1) We are ooking for some matrix and some transation vector A =(a jk ) j,k=1,...,n (2) t =(t 1,...,t n ) T (3) such that p i Aq i + t (i =1,...,m). (4) Asthe number of unknownsisn 2 +n, werequirem>n 2 +n. One possibe objective function to be minimized is the sum of squared Eucidean distances, i. e. S(A, t) = p i Aq i t 2 2. (5) The first soution method wi consist of a generaization of the east square fitting by a straight ine (n = 1). The second method is an iteration method that coud aso be appied but shoud not. Department of Mathematics, University of Odenburg, Postfach 2 503, D-26111 Odenburg, Germany, e-mai: spaeth@mathematik.uni-odenburg.de

28 H. Späth If A isorthogona, we wi have the n(n +1)/2 side conditions A T A = I, i. e. a T j a k = δ jk (j k) (6) where a j (j =1,...,n) are the coumnsof A. It wi turn out in Section 3 that it is easier to manage them impicity and that the mentioned second method can be used here. Other methods are discussed in [1, 2, 4, 5]. 2. Fitting affine transformations The necessary and because of inearity aso sufficient conditions for (5) to be minimized are S = 2 (E jk q i ) T (p i Aq i t) =0 (j, k =1,...,n) (7) a jk S t = 2 (p i Aq i t) =0 (8) In (7) we set E jk = A a jk,i.e.then n matrix that contains1 in the j-th row and the k-th coumn and 0 esewhere. As (E jk q i ) T =(0,...,0,q ki, 0,...,0), (9) where q ki isin the j-the position, the conditions (7) wi read ( m ) ( m ) ( m ) q 1i q ki a j1 +...+ q ni q ki a jn + q ki t j = q ki p ji (10) (j, k =1,...,n). Additionay, (8) gives ( m ) ( m ) q 1i a j1 +...+ q ni a jn + mt j = p ji (11) (j =1,...,n). In order to integrate (10) and (11) we introduce q n+1,i =1 (i =1,...,m) (12) and put q i =(q 1i,...,q ni,q n+1,i ) T (i =1,...,m), (13) Q = q i q T i, (14) ãa j =(a j1,...,a jn,t j ) T, (15) c j =( c j1,..., c j,n+1 ) T with c jk = q ki p ji (k =1,...,n+1). (16)

Fitting transformations 29 Then (10) and (11) can be integrated within Qãa j = c j (j =1,...,n). (17) Note that Q iscommon to a n systems of inear equations with n + 1 unknowns, i. e. you need just one LU-decomposition to sove a systems. Q wi normay be positivey definite for m>n 2 + n and thusnonsinguar. Exampe 1. For Q we used m =20points q i R 3 given by 0 1 0 1 1 0 1 1 1 1 1 1 1 1 0 1 1 1 0 0 Q = 0 0 1 1 0 1 1 0 0 0 1 1 0 1 0 1 1 0 1 1 1 0 0 0 1 1 1 0 1 1 0 1 1 0 1 1 1 1 1 1 Then we used A = 1 0 1 0 1 1, t = 1 0 1 1 0 1 to produce p i = Aq i + t (i =1,...,20). In this case the minima soution of (5) must give S(A, t) =0. Of course, this was done, and A and t were retrieved. Exampe 2. We disturbed a ot of coefficients of p i and q i randomy by ±1 to receive 0 1 0 0 1 1 1 1 1 1 1 0 0 1 0 1 0 1 1 0 Q = 1 1 1 1 0 1 0 1 1 1 1 1 1 1 1 1 1 1 1 1 1 0 1 1 1 1 1 0 1 1 0 1 1 0 1 1 0 0 1 1 1 0 1 0 1 2 2 3 1 3 1 3 1 2 1 1 1 1 2 0 P = 1 1 2 1 1 0 2 0 2 1 1 1 1 1 1 3 1 0 1 1 0 1 1 2 2 3 1 1 1 1 1 1 0 0 2 0 1 2 1 1 We received A =.6564.1728.5658.0028.7831 1.0776.7316.3747.1107, t = 1.1058.2724 1.0702 and S(A, t) =32.25425. Now we wi mention an iterative descent method that, it is true, does not exceed the straightforward and direct soution of (13) but wi aso be abe to be appied in the next section. We can write (8) as t = 1 m (p i Aq i ) (18) and (7) as (E jk q i ) T Aq i = (E jk q i ) T (p i t) (19) We consider the foowing agorithm:

30 H. Späth Step 0: Give some starting vaue A (0) for A, e.g.a (0) = I. Setw =0. Step 1: Use (18) to cacuate t (w+1) = 1 m (p i A (w) q i ). (20) Step 2: Use (19) to cacuate A (w+1),i.e.tosove (E jk q i ) T A (w+1) q i = (E jk q i ) T (p i t (w+1) ). (21) Step 3: STOP, if some convergence criterion is fufied, otherwise set w := w +1 and go back to Step 1. Thisaternating method givesa descent within every iteration. For the above two exampes it converged to 6 correct digits within 6 and 9 iterations, respectivey, and gave the same soution as (17). 3. Fitting orthogona transformations Orthogona transformations are affine transformations with the property (6). Thus to the objective function (5) one coud add the side conditions (6). Instead of trying to sove a noninear system after introducing the Lagrangian function we wi describe a more effective way. It is we-known [3] that every orthogona matrix A of size n n can be written asa product A = R 1 R N B, (22) where R = R(ϕ jk ) ( =1,...,N = and where R(ϕ jk )=(r is ) i,s=1,...,n hasthe eements (n 1)n ) (23) 2 r jj = r kk =cos(ϕ jk ) r jk = r kj = sin(ϕ jk ) (24) r ii =1 (i j, k), r is = 0 ese. The indices uniquey correspond to pairs (j, k) with j < k asindicated in the foowing tabe: 1 2 n 1 n n+1 2n 32n 2 N (j, k) (1, 2) (1, 3) (1,n)(2, 3) (2, 4) (2,n) (3, 4) (n 1,n)

Fitting transformations 31 Finay, B = I (identity) for det A = +1 [3, 6] and B =diag(1, 1,...,1, 1) for det A = 1 [3]. The anges ϕ ik are caed the Euer rotation anges. We wi aso write ϕ =(ϕ 1,...,ϕ N ) T With thisnotation the objective function (5) to be minimized here reads S(ϕ, t) = p i R 1 R 2 R N Bq i t 2 2. (25) The necessary conditions for a minimum are S m t = 2 (p i R 1 R N Bq i t) =0, (26) S ϕ = 2 i?1 (p i R 1 R N Bq i t) T R 1 R 1 R R +1 R N Bq i = 0 (27) where the matrix hasthe coefficients ( =1,...,N), R = R ϕ jk (28) r jj = r kk = sin(ϕ jk ), r jk = r kj = cos(ϕ jk), (29) r is = 0 ese. Note that the matrix C = R T R =(c is ) i,s=1,...,n (30) hasthe eements c jk = c kj = 1, c is = 0 ese. (31) Now(26)canbewrittenas t = t(ϕ) = 1 (p i R 1 R N Bq i ) m (32) and (27) as (p i t) T R 1 R R N q i = q T i RT N R T 1 R 1 R R N q i = = s T i RT R s i (33) s T i C s i i=2

32 H. Späth where s i = R +1 R N Bq i. But because of (31) the right-hand side of (33) is zero. Thus(27) reducesto Putting (p i t) T R 1 R 1 R R +1 R N Bq i =0. (34) u ()T i = (p i t) T R 1 R 1, v () i = R +1 R n Bq i, (i =1,...,n; =1,...,N) (35) (34) reads Using (29) this resuts in u ()T i R v () i = 0 (36) g jk sin(ϕ jk ) f jk cos(ϕ jk )=0, (37) where f jk = g jk = v () ij u() ik v() ik u() ij, v () ij u() ij + v() ik u() ik. (38) Thus ϕ ik = ϕ isgiven by ϕ ik =atan ( fjk A minimum of S w.r.t. ϕ jk isgiven by (39) if g jk ). (39) 1 2 2 S ϕ 2 ik = g jk cos(ϕ jk )+f jk sin(ϕ jk ) > 0. (40) Otherwise ϕ jk hasto be repaced by ϕ jk +π. Additionay, in order to avoid negative anges, we repace ϕ jk by ϕ jk +2π. Atogether we can now design the foowing descent agorithm: Step 1: Give starting vaues ϕ (0) ( =1,...,N), e.g. ϕ (0) = 0. Decide whether to use B = I or B =diag(1,...,1, 1). Set w =0. Step 2: Step 3: Cacuate R (w) = R(ϕ (w) )( =1,...,N) corresponding to (23) and (24). Set F := R (w) 2 R (w) N and G := I.

Fitting transformations 33 Step 4: Corresponding to (32) cacuate t (w) = 1 m (p i R (w) 1 Fq i ) Step 5: do =1,N end g := 0; f := 0; if = N then F := I do i =1,m u T := (p i t (w) ) T G v := Fq i g := g + v j u k v k u j f := f + v j u j + v k u k end i ϕ =atan(g/f) if (g cos(ϕ)+f sin(ϕ)) 0thenϕ := ϕ + π if (ϕ <0) then ϕ := ϕ +2π ϕ (w+1) := ϕ; R (w+1) if ( <n)then end if := R(ϕ) G := GR (w+1) ; F := R (w)t +1 F Step 6: Set w := w +1. If some convergence criterion is not fufied, then go back to Step 3; otherwise set t := t (w) and A := R (w) B and stop. 1 R (w) N Convergence of thisagorithm to a goba minimum cannot be proved. However, empiricay, the goba minimum wasawaysattained independenty of the starting vauesfor ϕ (0). We wi give some exampes where we aways used ϕ (0) =0( = 1,...,N). Starting with a set Q of m =20pointsa i R 4,namey Q = 1 1 1 1 1 1 0 0 0 0 0 0 0 1 1 0 0 0 2 2 0 1 1 1 1 0 0 1 1 1 1 0 0 0 0 0 2 2 2 2 0 0 1 1 0 0 0 0 1 1 0 1 1 1 1 2 0 2 2 2 0 0 0 1 1 1 1 1 1 0 0 0 1 1 0 0 0 0 2 0 and anges ϕ = ( =1,...,6) and a transation t =( 1, 0, 1, 2) T we produced p i = R 1 R 6 q i + t (i =1,...,m= 20). Exampe 3. Using those data after 206 iterations we got S =0.00000 (as expected) and t =( 1.0000, 0.0000, 1.0000, 2.0000) T ; instead of ϕ = ( =1,...,6) weendedupwithϕ 1 =1.0000, ϕ 2 =5.1416, ϕ 3 =.1416, ϕ 4 =5.4248, ϕ 5 =

34 H. Späth 1.8584, ϕ 6 =6.0000. This resut is right because with (ϕ 1,...,ϕ 6 ) T (among others) (ϕ 1,ϕ 2 + π, π ϕ 3, 3π ϕ 4,ϕ 5 π, ϕ 6 ) T is aso a goba minimum. Exampe 4. We used the same data as before but dropped a components of p i from d 1.d 2 d 3 d 4 d 5 d 6 to d 1.d 2 thus introducing sma errors. After 202 iterations we received S = 0.07328, t =(.9644,.0459,.9469, 1.9441) T and ϕ = (.9614, 5.1497,.1431, 5.3838, 1.8640, 5.9972) T. As expected, these resuts do not differ very much from those of Exampe 3. Exampe 5. We further dropped the components of p i from d 1.d 2 to integer vaues d 1 getting P = 0 0 1 0 0 0 0 0 0 1 0 1 0 0 1 2 0 1 0 1 0 0 1 1 0 0 0 0 1 0 0 0 1 1 1 1 0 1 3 2 0 0 0 0 0 0 1 1 1 1 1 1 1 0 0 1 1 1 0 0 2 3 3 2 2 1 1 2 2 3 2 2 1 1 2 2 3 4 3 4 After 258 iterations we got S =5.66304, t =(.5893,.5366,.6593, 1.6014) T and ϕ =(1.3334, 5.0294,.1224, 5.5977, 2.0565, 6.0189) T. Of course, these resuts differ more than before. Varying the starting vaues ϕ (0) we aways received the same resuts, i.e. hopefuy a goba minimum. References [1] J. C. Gower, Mutivariabe anaysis: Ordination, mutidimensiona scaing and aied topics, in: Statistics, Handbook of Appicabe Mathematics, Vo. VI, (E. H. Loyd, Ed.), Wiey, Chichester, 1984, 727-781. [2] R. J. Hanson, M. J. Norris, Anaysis of measurements based on the singuar vaue decomposition, SIAM J. Sci. Statist. Comput. 2(1981), 363 373. [3] F. Neiss, Determinanten und Matrizen, 2. Aufage, Springer, 1967. [4] P. H. Schönemann, R. M. Carro, Fitting one matrix to another under choice of a centra diation and a rigid motion, Psychometrika35(1970), 245 255. [5] I. Söderkvist, P.-Å. Wedin, On condition numbers and agorithms for determining a rigid body movement, BIT 34(1994), 424 436. [6] N. JA. Vienkin, Specia Functions and the Theory of Group Representations, AMS, Providence 1968.