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The method

We have separated r and E, from direction variables and turned integration to

summation for direction in the scatter source

)(

)

(

(

(

ˆ

P pq

 

)2('

) (

)

(

)

(

(

1

1 4

, ,

,

, ,

,

 

  

dE mY

l

E

E E

E

pr r

p

scat q

ErE t

ErE

)3(

)ˆ ˆ( )ˆ ˆ(

1

)ˆ ˆ

(

2/1 )

(

0 0

,

,

,

,

,

, ,



 



 

 

d

P

E E

E E

l

l

l m

rml

rls

r scat

q

)4(

'

)ˆ(

)ˆ, ,(

) ,(

1

,

,

,

,





 





d m

lY Er

Erml

l

rs

rls

Let us continue with E

4

,