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The intensity operator represents a sum of contrillll t ion from t 1\(, san\(' scatterer as represented by the first t('rm in (~)A.22) and from diff('H'nt scatterers weighted by Tl. s ./ '(Ls/ h s I'"~ (1') - 1'1) as 1'('j>l'('s('nt('d by t!H' second term in (5.4.22). As noted, G j repn'sents transition scattering matrix of the jth scatterer in the presence of ot!H'r scatterers. It is interesting to compare (5.4.22) with the usually ladder approximation. In the usual ladder approximation. th(' second term in (5.4.22) is absent and secondly C/ in (5.4.22) is replaced by Til which is the transition matrix of the lth particle in the abs('ncc of other scatterers. Obviously, the two cases reduce to each other for sparse concentration of particles when Tl. s ] n Sl h sjs , can be neglected and G/ is approximately equal to T I .



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In this section, we illustrate the derivation of the radiative transfer equation from the ladder approximation. To simplify the derivation, we use isotropic point scatterers. We assume that the extinction coefficient of the coherent wave is much smaller than the wavenumber. Consider a wave 'lj)inc("r) incident on a single point scatterer located at l'a' Then the total field 'lj) is given by

'1/)(1') = 'lj)inc(r)

eiklr-r,,1

1'lj)inc(ra )

(5.5.1)

where f is the scattering amplitude and k is the wavenumber of the background medium. Since C(O)(r) = exp(ih)j41IT is the Green's function for the unperturbed problem, (5.5.1) can be written as

'ljJ(r)

= 'ljJinc(r) + ./df'





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C(O) (1', r')To,{r', 1''')'ljJinc ("r")

(5.5.2)

Tn (1", 1''') = 47f f 0(1" - 1'0') 0(1''' - 1'0')

is the transition operator for the point scatterer at C (I)) (1' 1") = -(-,'----;-:, 47flr oiklr-r'l

(5.5.3)

We also use (5.5.4)

In diagrammatic notation, let (5.5.5) Then (5.5.2) becomes '1/) =

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