26.12.2013 Views

Coherent Backscattering from Multiple Scattering Systems - KOPS ...

Coherent Backscattering from Multiple Scattering Systems - KOPS ...

Coherent Backscattering from Multiple Scattering Systems - KOPS ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

5.1 Conservation of energy in coherent backscattering<br />

1<br />

kl* = 2<br />

kl* = 4<br />

kl* = 10<br />

0.8<br />

cooperon<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−90 −60 −30 0 30 60 90<br />

scattering angle [deg]<br />

Figure 5.5: Old and new theory. The graph shows the cooperon calculated with<br />

eqn. 2.15 (dashed lines) and including the additional contribution given in eqn. 5.7<br />

(solid lines). The dotted lines give the enhancement of the cooperon for the new theory<br />

(for the old theory the enhancement is always equal to 1). Parameters: wavelength<br />

λ = 590 nm, diffusion coefficient D = 15 m2 /s, reflectivity R = 0.5.<br />

The fit parameter a is therefore obtained by numerical integration of<br />

a =<br />

0<br />

∫ π/2<br />

0<br />

∫ π/2<br />

I (A)<br />

c<br />

1<br />

(kl ∗ ) 2 ·<br />

· sin θ dθ<br />

µ · sin θ dθ<br />

µ + 1<br />

After normalization analogous to eqns. 2.13, the additional contribution to the cooperon finally<br />

becomes<br />

α (B+C)<br />

c<br />

8π · a<br />

= −<br />

3 k 2 l ∗ (l ∗ + 2z 0 ) ·<br />

µ<br />

µ + 1<br />

(5.7)<br />

does not contribute at a specific angular value but it is rather spread out over the<br />

whole angular range, similar to the diffuson. In particular it reduces the enhancement of the<br />

coherent backscattering cone, so that the total cooperon α (A)<br />

c<br />

α (B+C)<br />

c<br />

+ α (B+C)<br />

c at the conetip at θ = 0<br />

51

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!