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Controlling light in scattering media

Controlling light in scattering media

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The scatter<strong>in</strong>g matrix<br />

Our system of study: A thick (opaque) layer of ZnO on a slab<br />

• Very stable (stationary diffuser, stable speckle figure)<br />

• Completely disordered, <strong>in</strong> the multiple scatter<strong>in</strong>g regime<br />

• L<strong>in</strong>ear, open system<br />

A natural formalism: the scatter<strong>in</strong>g matrix<br />

A <strong>in</strong><br />

A out<br />

t<br />

L<strong>in</strong>k the <strong>in</strong>put to the output fields of the system<br />

Bout B B <strong>in</strong><br />

<br />

A<strong>in</strong><br />

B <strong>in</strong><br />

=<br />

<br />

r<br />

t<br />

t <br />

.<br />

r<br />

<br />

Scatter<strong>in</strong>g matrix S<br />

<br />

Aout<br />

B out<br />

The transmission matrix (TM)<br />

can be measured with a CCD and a SLM!

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