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Modal Analysis<br />

• Modal Decomposition<br />

E( x,<br />

y,<br />

z)<br />

= ∑ a<br />

m<br />

m<br />

E<br />

m<br />

( x,<br />

y,<br />

z)<br />

with<br />

⎡ ∂<br />

⎢<br />

⎣∂x<br />

2<br />

2<br />

+<br />

∂<br />

2<br />

∂y<br />

2<br />

+<br />

k<br />

2<br />

0<br />

n<br />

2<br />

( x,<br />

⎤<br />

y,<br />

z)<br />

⎥ E<br />

⎦<br />

m<br />

( x,<br />

y,<br />

z)<br />

=<br />

β ( x,<br />

2<br />

m<br />

y,<br />

z) E<br />

m<br />

( x,<br />

y,<br />

z)<br />

• Approximate Forward Solution<br />

E(<br />

∑<br />

−iβ<br />

m ( x,<br />

y,<br />

z ) ∆z<br />

x,<br />

y,<br />

z + ∆z)<br />

= e E<br />

m<br />

( x,<br />

y,<br />

z)<br />

m<br />

<strong>Faculty</strong> <strong>of</strong> <strong>Science</strong> - Department <strong>of</strong><br />

Physics 5/3/2009<br />

D. Yevick - Evolution Operators and<br />

Boundary Conditions<br />

7

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