Difference between revisions of "Attenuated Total Reflectance"

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The electro-optic coefficient for a poled polymer film can be calculated as follows.
The electro-optic coefficient for a poled polymer film can be calculated as follows.


:<math>r_{33} = \frac {2d\Delta R}  {n^3_{TM} V_m}  \frac {\delta n_{eff}} {\delta \theta} \left {/(}   \frac {\delta R \delta n_{eff} }  {\delta \theta \delta n_{TM} } \right )  \,\!</math>
:<math>r_{33} = \frac {2d\Delta R}  {n^3_{TM} V_m}  \frac {\delta n_{eff}} {\delta \theta} \left /(  \frac {\delta R \delta n_{eff} }  {\delta \theta \delta n_{TM} } \right )  \,\!</math>


where
where

Revision as of 15:08, 12 January 2010

Overview

Attenuated Total Reflection or ATR is a technique used together with Teng Mann to measure the R33 of electro-optic materials.

Technique

Significance

The electro-optic coefficient for a poled polymer film can be calculated as follows.

<math>r_{33} = \frac {2d\Delta R} {n^3_{TM} V_m} \frac {\delta n_{eff}} {\delta \theta} \left /( \frac {\delta R \delta n_{eff} } {\delta \theta \delta n_{TM} } \right ) \,\!</math>

where

<math>n_{TE}\,\!</math> is the ordinary index of refraction
<math>n_{TM}\,\!</math> is the extraordinary index of refraction
<math>E\,\!</math> is the modulating electric field

References