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This document recounts the story of Professor Gene Golub's encounter with the Secular Equation during his academic career. It includes his discovery of the minimal norm solution for rank deficient matrices and his work on least squares problems with quadratic constraints. The document also mentions his collaboration with other researchers and his influential papers on the topic.
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My First Encounter with Prof. Gene H. Golub (1932 – 2007)
Walter Gander, ETH and HKBU
International Workshop on Matrix Computations Gene Golub Memorial Day 2018 Hangzhou April 20 – 24, 2018
m=40; A=magic(m); n=m/5; A=A(:,1:n); b=A*rand(n,1); Solutions : Matlab A\b Using SVD Extrapolation Warning: Rank deficient with rank r = 3 4 iterations 1.846673326583244 0.457727535991772 0. 2.459131966980111 0.747175086297768 0. 0 0.694218248476673 0. 0 0.616598049455061 0. 0 0.669554887276158 0. 0 0.535347735013380 0. 0 0.482390897192287 0. 0.725632546879197 0.828425400739452 0.
Norm of solutions: 3.159758693196030 1.812127976894189 1. Norm of residuals: 1.0e-10 * 0.055694948577711 0.136651389778460 0.
Peter Henrici Rudolf Kalman 1923 – 1987 1930 – 2016
ahttp://www.cs.cas.cz/~harrachov
(^2) i γ i^2 ,^ i^ = 1,... , r^ are the eigenvalues of generalised EV-Problem A>Ax = μC>Cx.
f (λ) =
∑^ r 1=
α^2 i
( (^) γ ici −^ αiei α^2 i + λγ i^2
) 2
∑^ p i=r+
e^2 i = δ^2
f has at most r poles for λ = −μi and f (λ) = δ^2 at most 2 r solutions
If (x 1 , λ 1 ) and (x 2 , λ 2 ) are solutions of the normal equations, then
Thm 1
‖Ax 2 − b‖^2 − ‖Ax 1 − b‖^2 = λ^1 − 2 λ^2 ‖C(x 1 − x 2 )‖^2.
If λ 1 > λ 2 =⇒ ‖Ax 1 − b‖ < ‖Ax 2 − b‖ =⇒ the largest solution λ determines solution
Thm 2
− λ^1 + 2 λ^2 ‖C(x 1 − x 2 )‖^2 = ‖A(x 1 − x 2 )‖^2. =⇒ λ 1 + λ 2 < 0 =⇒ At most one λ > 0
‖Ax − b‖^2 = min subject to ‖Cx − d‖^2 ≤ δ^2
A b 0.73980.8930 0.52440.7545 -4.4414-5. 0.02590.1376 0.16980.6727 -0.7691-2. 0.42410.7646 0.61870.0068 -1.1464-4.
C d -1.6443-0.0263 -1.9204-0.3913 2.26503. -1.9660 -0.2804 2.
‖Ax − b‖ = const, ‖Cx − d‖ = 10 f (λ) = ‖Cx(λ) − d‖
active constraint, λi = [− 0. 7857 , 0 .0772], poles= −μi = [− 0. 4582 , − 0 .2935]
A b 0.58590.1907 0.63090.8920 -3.9636-3. 0.50340.0509 0.67340.6853 -1.9904-5. 0.05610.3352 0.69570.7998 -1.4789-3.
C d -0.5194-1.4917 -0.9237-0.1797 3.74133. -0.3088 -1.2986 2.
‖Ax − b‖ = const, ‖Cx − d‖ = 10 f (λ) = ‖Cx(λ) − d‖ λi = [− 1. 6157 , − 0. 9211 , − 0. 1827 , − 0 .0962], poles = −μi = [− 1. 2686 , − 0 .1393]
A b 0.92000.9800 0.99000.8000 2.90002. 0.04000.8500 0.81000.8700 1.66002. 0.86000.1700 0.93000.2400 2.72000. 0.23000.7900 0.05000.0600 0.33000. 0.10000.1100 0.12000.1800 0.34000.
C = A
d 0.81470. 0.12700. 0.63240. 0.27850. 0.95750.
λi = [− 1. 4057 , − 0 .5943], −μi = [− 1. 0000 , − 1 .0000]