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Published byAustin Hardy Modified over 9 years ago
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Fiber Optics Design and Solving Symmetric Banded Systems
Linda Kaufman William Paterson University
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Dispersion Compensation fibers
Signal degradation and Restoration Transmission (~80km) Dispersion Compensation Amplification EDFA High Speed Optical Communication Segment
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Fiber Optics Design and Solving symmetric Banded systems
Linda Kaufman William Paterson University
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Marcuse model for fiber wrapped around spool
For a radially symmetric fiber where r is the radius from the center of the fiber, R is the radius of the spool which leads to a matrix problem of the structure. b’s and c’s are 0(r/R)
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Objective: Create a algorithm to factor a symmetric indefinite banded matrix A
An n x n matrix A is symmetric if ajk = akj A matrix is indefinite if any of these hold a. eigenvalues are not necessarily all positive or all negative b. One cannot factor A into LLT is indefinite- determinant is negative -5 2 A has band width 2m+1 if ajk = 0 for |k-j| >m m=2 x x x x x x x 0 x x x x x x x x x
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Uses (1)Solve a system of equations Ax=b If A = MDMT , D is block diagonal, one solves Mz=b Dy =z MTx =y (2)Find the inertia of a system- the number of positive and negative eigenvalues of a matrix If A = MDMT, The inertia of A is the inertia of D. Given a matrix B, the inertia of a matrix A = B-cI is the number of eigenvalues greater, less than and equal to c.
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Competition Ignore symmetry- use Gaussian elimination- does not give inertia info- 0(nm2) time-(n is size of matrix, m is bandwidth) Band reduction to tridiagonal (Schwarz,Bischof, Lang, Sun, Kaufman) followed by Bunch for tridiagonal-0(n2m) Snap Back-Irony and Toledo-Cerfacs-2004, 0(nm2) time generally faster than GE but twice space Bunch – Kaufman for general matrices and hope bandwidth does not grow as Jones and Patrick noticed
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Difficulties Consider the linear system .0001x + y = 1.0 x + y = 2.0
Gaussian elimination- 3 digit arithmetic 10000y = 10000 Giving y = 1, x =0 But true solution is about x =1.001, y =.999 If interchange first and second rows and columns before Gaussian elimination get x + y = 2.0 y = = 1.0 So x = 1.0- a bit better
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Gaussian elimination with partial pivoting to prevent division by zero and unbounded elemental growth Unsymmetric pivoting yields 0 x x x f 0 x x f f Eliminating first column yields 5 diagonal becomes 7 diagonal In general 2k+1 diagonal becomes 3k+1 diagonal
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Symmetric pivoting But pivoting tends to upset the band structure!!
But to maintain symmetry one must pivot rows and columns simultaneously What if matrix is ? 1 0 Interchanging first row and column does not help If matrix is Pivot it to And use top 2 x 2 as a “pivot” But pivoting tends to upset the band structure!!
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Bunch -Kaufman for symmetric indefinite non banded
Partition A as Where D is either 1 x 1 or 2 x 2 and B’ = B – Y D-1 YT Choice of dimension of D depends on magnitude of a11 versus other elements If D is 2 x 2, det(D)<0
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2 x 2 vs 1 x 1 for nonbanded symmetric system
x x x
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Bandwidth spread with Bunch-Kaufman on banded matrix
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Banded algorithm based on B-K
1) Let c = |ar 1 | = max in abs. in col. 1 2) If |a11 | >= w c, use a 1 x 1 pivot. Here w is a scalar to balance element growth, like 1/3 Else 3)Let f= max element in abs. in column r 4) If w c*c <= |a11 | f, use a 1 x 1 pivot 5)interchange the rth and second rows and columns of A 6) perform a 2 by 2 pivot 7) fix it up if elements stick out beyond the original band width Never pivot with 1 x 1
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Fix up algorithm Worst case r =m+1, what happens in pivoting
x x x x x x x x x x x x x a b c d x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x a x x x x x x x x x x b x x x x x x x x x x c x x x x x x x x x d x x x x x x x x x x x x x x x x x x x x x x x x x x x x x
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Partition A as If we don’t remove elements outside the band,
Reset B’ = B – Y D-1 YT Let Z = D-1 YT = x x x x x x x x x p q r s x x x x x . Then B’ looks like x x x x x x bp cp dp x x x x x x x cq dq x x x x x x x cr dr x x x x x as bs cs ds x x x x x x x x x x x x x x x x as x x x x x x x x bp x x bs x x x x x x x x cp cq x cs x x x x x x x x dp dq dr ds x x x x x x x x x x x x x x x x x x x x x x x x x x x x x If we don’t remove elements outside the band, the bandwidth could explode to the full matrix.
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Because of structure eliminating 1 element gets rid of column
x x x x x x x x x x x x x cq dq x x x x x x x cr dr x x x x x x bt ct dt x x x x x x x x x x x x x x x x x x x x x x x x bt x x x x x x x x cq cr ct x x x x x x x x dq dr dt x x x x x x x x x x x x x x x x x x x x x x x x x x x x x
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Continue with eliminating another element
x x x x x x x x x x x x x x x x x x x x x u x x x x x x x x m x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x u m x x x x x x x x x x x x x x x x x x x x x x x x x x x x x Now eliminate u to restore bandwidth
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In practice one would just use the elements in the first part of Z to determine the Givens/stabilized elementary transformations and never bother to actually form the bulge. Thus there is never any need to generate the elements outside the original bandwidth.
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Alternative Formulation
Partition A as Where D is 2 x 2 Let Z = D-1 YT Reset B’ = QT(B – Y Z)Q= QTB Q-HG Where H=QTY and G =ZQ Therefore do “retraction” followed by rank 2 correction. Recall H looks like h1 h2 0 h3 Where the “0” has length r-1 and the whole H has length m+r-1
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Alternative-2 Q is created such that G =ZQ has the form G =
where 0 has r-3 elements and G5 is a multiple of G3 1)Explicitly use 0’s in rank-2 correction Thus correction has form below where numbers indicate the rank of the correction (r-3 rows) (m-r+2 rows) (r-1 rows) 2) Store Q info in place of 0’s and G3 to reduce space to (2m+1)n 3) Reduce solve time for each 2 x 2 from 4m+6r mults to 4m+2r- In worst case, 3mn vs. 5mn
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Properties Space- (2m+1)n-in order to save transformations compared to (3m+1)n for unsymmetric G.E. Never pivots for positive definite or 1 x 1 Decrease operations by not applying second column of pivot when these will be undone Operation count depends on types of transformations Elementary –between m2n/2 and 5 m2n/4 Compared with between m2n and 2m2n for G.E.
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Elemental growth Let a = max element of matrix
For 1 x 1, Ajk = Ajk – A1k Aj1 /A11 taking norms element growth is a(1+1/w) For 2 x 2 if no retraction, it turns out that element growth after 1 step is a(1 + (3+w)/(1-w)) For 2 x 2 if retraction, it turns out that element growth is (4+8/(1-w))a 2 steps of 1 x 1 = 1 step of retraction when w=1/3, giving growth bound of 4n-1
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Comparison using Atlas Blas on Sun
Problem 1 2 3 4 Time-retraction (ms)elem/orthog 98/98 161/240 296/520 220/220 Time-Snapback elem/orthog 140/140 550/590 1640/ 2200 1290/1370 Time-Lapack-tf2/trf 195/136 395/235 Error-retraction 3e-15 /3e-15 1.6e-13 /1.3e-13 3e-13/ 9e-14 2e-11 /5e-12 Error-snapback 5e-15 /5e-15 4e-11 1e-13 2.2e-4 4e-12 3e-5 Error Lapack-tf2 7e-15 1e-15 6e-15 1e-12
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Retraction vs. Lapack
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Elementary Orthogonal Time 150 160 2 x2’s 204 179 error 3.04e-11
Elementary vs. orthogonal on 2 random matrices, n=1000, m=100 Elementary Orthogonal Time 150 160 2 x2’s 204 179 error 3.04e-11 1.10e-11 growth 146.4 1292.1 221 178 1.00e-12 3e-12 130.5 1762.8 I thought orthogonal would be more accurate, have less elemental growth, and take much more time-but these assumptions were wrong for random matrices
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Future Could do pivoting with 1 by 1 at price of space and time- needs to be implemented Adaptations for small bandwidth as in optical fiber code. Condition estimator
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