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Frequency domain seismic forward modelling: A tool for waveform ...

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U 11<br />

0<br />

U 15<br />

L 11<br />

U 55<br />

U 22<br />

U 25<br />

L 22<br />

L 33<br />

L 44<br />

U 33<br />

0<br />

U 35<br />

U 44<br />

L 15 L 25 L 35 L 45<br />

L 55<br />

U 45<br />

Figure 2.3: Two way dissected matrix S ~<br />

= L ~<br />

U ~<br />

. During LU decomposition the<br />

values <strong>for</strong> L i;j and U i;j are lled in at the corresponding locations used by S i;j . L i;j<br />

and U i;j denotes possible non-zero elements in matrices L ~<br />

and U ~<br />

respectively after<br />

LU decomposition while 0 denotes zero elements.<br />

the amounts necessary to per<strong>for</strong>m LU decomposition on the n 2<br />

by n 2 grids (L i;i), plus<br />

L 5;i which comes from the coupling between the elements within each subgrid and<br />

the elements within the dissector. In the rst dissection one can write the memory<br />

requirements as:<br />

S(n; 0) = 4S(n=2; 2) + D(n; 0) (2.9)<br />

where S(i; j) represents memory requirement <strong>for</strong> the subgrid of size i bordered by<br />

n<br />

n<br />

n<br />

n<br />

n<br />

n<br />

S(n,2) S(n,3) S(n,4)<br />

Figure 2.4: All possible subgrid (S(n; 2);S(n; 3) and S(n; 4)) situations arising during<br />

nested dissection. The thick black borders represent neighbouring dissectors<br />

from previous dissections in the recursion.<br />

45

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