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Analysis of the extended defects in 3C-SiC.pdf - Nelson Mandela ...

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43<br />

beam left-hand side g' = 0 g' = g<br />

g<br />

d 0<br />

<br />

e<br />

0: 2 is 0<br />

0 0 i <br />

'<br />

g (4.15)<br />

dz<br />

<br />

q<br />

0<br />

i g<br />

d g<br />

e<br />

<br />

g: 2 is g<br />

g i 0 ' g<br />

(4.16)<br />

dz<br />

q <br />

These equations may be written <strong>in</strong> <strong>the</strong> form,<br />

dT<br />

dz<br />

dS<br />

dz<br />

i<br />

isgT<br />

S ; (4.17)<br />

q<br />

g<br />

i<br />

is g S T ; (4.18)<br />

q<br />

g<br />

by means <strong>of</strong> <strong>the</strong> follow<strong>in</strong>g substitution,<br />

)<br />

z<br />

0 T ( z e ; (4.19)<br />

i<br />

g z<br />

g S(<br />

z e e ; (4.20)<br />

)<br />

i<br />

with i(<br />

s ) ' g . This is done to remove <strong>the</strong> dependence on <strong>the</strong> normal<br />

<br />

0<br />

absorption length and to render <strong>the</strong> equations more symmetric. Thus follow<strong>in</strong>g this<br />

procedure <strong>the</strong> solution to <strong>the</strong> problem is derived as follows. Equation 4.17 is written<br />

as,<br />

q<br />

g dT<br />

S s gq<br />

gT<br />

; (4.21)<br />

i<br />

dz<br />

and<br />

dS<br />

dz<br />

2 q<br />

g d T<br />

sg<br />

q<br />

i<br />

dz<br />

2<br />

g<br />

dT<br />

dz<br />

g<br />

i <br />

g<br />

0<br />

(4.22)

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