Fiber Optics Design and Solving Symmetric Banded Systems

28
Fiber Optics Design and Solving Symmetric Banded Systems Linda Kaufman William Paterson University

description

Fiber Optics Design and Solving Symmetric Banded Systems. Linda Kaufman William Paterson University. High Speed Optical Communication Segment. EDFA. Dispersion Compensation. Amplification. Transmission (~80km). Dispersion Compensation fibers. Signal degradation and Restoration. - PowerPoint PPT Presentation

Transcript of Fiber Optics Design and Solving Symmetric Banded Systems

Page 1: Fiber Optics Design and Solving Symmetric Banded Systems

Fiber Optics Design and Solving Symmetric Banded

Systems

Linda Kaufman

William Paterson University

Page 2: Fiber Optics Design and Solving Symmetric Banded Systems

Dispersion Compensation fibers

Signal degradation and Restoration

Transmission (~80km)Dispersion

CompensationAmplification

EDFA

High Speed Optical Communication Segment

Page 3: Fiber Optics Design and Solving Symmetric Banded Systems

Fiber Optics Design and Solving symmetric Banded systems

Linda Kaufman

William Paterson University

Page 4: Fiber Optics Design and Solving Symmetric Banded Systems
Page 5: Fiber Optics Design and Solving Symmetric Banded Systems

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)

Page 6: Fiber Optics Design and Solving Symmetric Banded Systems

705020

503010

20101

Objective: Create a algorithm to factor a symmetric indefinite banded matrix A

An n x n matrix A is symmetric ifajk = 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 1 -5 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 x

x x x x x

0 x x x x

x x x

Page 7: Fiber Optics Design and Solving Symmetric Banded Systems

Uses

(1)Solve a system of equations Ax=bIf A = MDMT , D is block diagonal, one solves

Mz=bDy =zMTx =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-cIis the number of eigenvalues greater, less than and equal

to c.

Page 8: Fiber Optics Design and Solving Symmetric Banded Systems

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

Page 9: Fiber Optics Design and Solving Symmetric Banded Systems

Consider the linear system.0001x + y = 1.0x + y = 2.0

Gaussian elimination- 3 digit arithmetic.0001x + y = 1.010000y = 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 = 2.0 -1.0= 1.0

So x = 1.0- a bit better

Difficulties

Page 10: Fiber Optics Design and Solving Symmetric Banded Systems

Gaussian elimination with partial pivoting to prevent division by zero and unbounded elemental growth

1 1 101 8 4 610 4 3 5 8 6 5 7 1 3 8 1 6 2 1 3 2 5 4 1 4 7

Unsymmetric pivoting yields

10 4 3 5 8 1 8 4 61 1 10 6 5 7 1 3 8 1 6 2 1 3 2 5 4 1 4 7

Eliminating first column yields

10 4 3 5 8 0 x x x f0 x x f f 6 5 7 1 3 8 1 6 2 1 3 2 5 4 1 4 7

5 diagonal becomes 7 diagonal

In general 2k+1 diagonal becomes 3k+1 diagonal

Page 11: Fiber Optics Design and Solving Symmetric Banded Systems

Symmetric pivoting

But to maintain symmetry one must pivot rows and columns simultaneouslyWhat if matrix is

0 1 ?1 0

Interchanging first row and column does not help

If matrix is0 1 10001 0 101000 10 0

Pivot it to 0 1000 11000 0 101 10 0

And use top 2 x 2 as a “pivot”

But pivoting tends to upset the band structure!!

Page 12: Fiber Optics Design and Solving Symmetric Banded Systems

Bunch -Kaufman for symmetric indefinite non banded

Where D is either 1 x 1 or 2 x 2and 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

Partition A as

Page 13: Fiber Optics Design and Solving Symmetric Banded Systems

2 x 2 vs 1 x 1 for nonbanded symmetric system

4 2 1 1 0 0 2 3 3 1 x 1 0 2 2.5

1 3 5 0 2.5 4.75

1 10 5 1 0 0 10 200 3 1 x 1 0 100 -47 5 3 8 0 -47 -17

1 10 5 1 10 0 10 50 3 2 x 2 10 50 0 5 3 8 0 0 25.3

Page 14: Fiber Optics Design and Solving Symmetric Banded Systems

Bandwidth spread with Bunch-Kaufman on banded matrix

Page 15: Fiber Optics Design and Solving Symmetric Banded Systems

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

Else5)interchange the rth and second rows and columns of A6) perform a 2 by 2 pivot7) fix it up if elements stick out beyond the original band width

Never pivot with 1 x 1

Page 16: Fiber Optics Design and Solving Symmetric Banded Systems

Fix up algorithm

Worst case r =m+1, what happens in pivotingx x x x x xx x x x x x x a b c dx x x x x x x xx x x x x x x x xx x x x x x x x x xx 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

Page 17: Fiber Optics Design and Solving Symmetric Banded Systems

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 dpx x x x x x x cq dqx x x x x x x cr drx x x x x as bs cs ds x x x x x x x x x x x x xx x x as x x x x x x x xbp x x bs x x x x x x x xcp cq x cs x x x x x x x xdp 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 xIf we don’t remove elements outside the band, the bandwidth could explode to the full matrix.

Partition A as

Page 18: Fiber Optics Design and Solving Symmetric Banded Systems

Because of structure eliminating 1 element gets rid of column

x x x x x xx x x x x x x cq dqx x x x x x x cr drx 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

Page 19: Fiber Optics Design and Solving Symmetric Banded Systems

Continue with eliminating another element

x x x x x xx x x x x x x x x x x x x x x ux 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

Page 20: Fiber Optics Design and Solving Symmetric Banded Systems

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.

Page 21: Fiber Optics Design and Solving Symmetric Banded Systems

Alternative Formulation

Partition A asWhere D is 2 x 2

Let Z = D-1 YT

Reset B’ = QT(B – Y Z)Q= QTB Q-HGWhere H=QTY and G =ZQTherefore 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

Page 22: Fiber Optics Design and Solving Symmetric Banded Systems

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 correctionThus correction has form below where numbers indicate the rank of the correction 1 1 0 (r-3 rows) 1 2 1 (m-r+2 rows) 0 1 1 (r-1 rows)2) Store Q info in place of 0’s and G3 to reduce space to (2m+1)n3) Reduce solve time for each 2 x 2 from 4m+6r mults to 4m+2r- In worst case, 3mn vs. 5mn

G G G

G G

1 2 3

0 4 5

Page 23: Fiber Optics Design and Solving Symmetric Banded Systems

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.

Page 24: Fiber Optics Design and Solving Symmetric Banded Systems

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

Page 25: Fiber Optics Design and Solving Symmetric Banded Systems

n=1000, m=100 problem diagonal offdiagonal outer diagonal pos. eigenvalues

/2x2/average r 1 100 1 1 1000/0/0/ 2 10 1 100 502/161/66 3 10 1 10000 500/500/89 4 1 10*|i-j| 10*|i-j| 493/397/57

Problem 1 2 3 4

Time-retraction (ms)elem/orthog

98/98 161/240 296/520 220/220

Time-Snapbackelem/orthog

140/140 550/590 1640/2200

1290/1370

Time-Lapack-tf2/trf 195/136 395/235 395/235 395/235

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-52e-11

Error Lapack-tf2 7e-15 1e-15 6e-15 1e-12

Comparison using Atlas Blas on Sun

Page 26: Fiber Optics Design and Solving Symmetric Banded Systems

Retraction vs. Lapack

Lapack vs. retraction, n=2000, on random matrices, with about 1000 + eigenvalues

0

5

10

15

20

25

30

0 100 200 300 400 500 600

half bandwidth

tim

e

dgbtrf

retraction

dgbtf2

Page 27: Fiber Optics Design and Solving Symmetric Banded Systems

Elementary Orthogonal

Time 150 160

2 x2’s 204 179

error 3.04e-11 1.10e-11

growth 146.4 1292.1

Time 160 160

2 x2’s 221 178

error 1.00e-12 3e-12

growth 130.5 1762.8

Elementary vs. orthogonal on 2 random matrices, n=1000, m=100

I thought orthogonal would be more accurate, have less elemental growth, and take much more time-but these assumptions were wrong for random matrices

Page 28: Fiber Optics Design and Solving Symmetric Banded Systems

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