Difference between revisions of "Teng-Man Method"
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[[Image:teng_mann.png|thumb|500px|Teng-Man Testing configuration]] | [[Image:teng_mann.png|thumb|500px|Teng-Man Testing configuration]] | ||
We use the Teng - Man method to measure R<sub>33</sub>. | We use the Teng - Man method to measure R<sub>33</sub>. | ||
R<sub>33</sub> is an elipsometric measurement<ref>http://en.wikipedia.org/wiki/Ellipsometry</ref>. You apply a voltage to the film while making the elipsometric measurements and looking for changes in the signal. | R<sub>33</sub> is an elipsometric measurement<ref>http://en.wikipedia.org/wiki/Ellipsometry</ref>. You apply a poling voltage to the film while making the elipsometric measurements and looking for changes in the signal. The stage can be heated until the film reaches its melting point T<sub>g</sub>. These measurements are made with the materials in a device configuration. The formula for R<sub>33</sub> | ||
:<math>r_{33}= \frac {3\lambda I_m } {4 \pi V_{poly}I_c n^2 } \frac {(n^2 - sin^2 \theta) ^{1/2}}{sin^2 \theta} \approx I_m/ I_c | :<math>r_{33}= \frac {3\lambda I_m } {4 \pi V_{poly}I_c n^2 } \frac {(n^2 - sin^2 \theta) ^{1/2}}{sin^2 \theta} \approx I_m/ I_c | ||
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[[Image:Teng mann graph.png|thumb|400px|right|Real time optimization of r<sub>33</sub>]] | [[Image:Teng mann graph.png|thumb|400px|right|Real time optimization of r<sub>33</sub>]] | ||
Teng_Mann techniques allows real-time optimization of processing conditions because you can evaluate r<sub>33</sub> during the poling process. | Teng_Mann techniques allows real-time optimization of processing conditions because you can evaluate r<sub>33</sub> during the poling process. It is used to confirm that a sample has been poled. The R33 measurement is best used as a relative measure because it can be inaccurate. Use attenuated total reflection ATR to get an accurate absolute measure. | ||
Revision as of 13:25, 7 January 2010
Teng-Mann Method for Measuring Electro-optic coefficient
We use the Teng - Man method to measure R33. R33 is an elipsometric measurement[1]. You apply a poling voltage to the film while making the elipsometric measurements and looking for changes in the signal. The stage can be heated until the film reaches its melting point Tg. These measurements are made with the materials in a device configuration. The formula for R33
- <math>r_{33}= \frac {3\lambda I_m } {4 \pi V_{poly}I_c n^2 } \frac {(n^2 - sin^2 \theta) ^{1/2}}{sin^2 \theta} \approx I_m/ I_c
\,\!</math> where
- <math>I_m\,\!</math> is the amplitude of modulation
- <math>V_{poly}\,\!</math> is the modulation voltage across EO polymer
- <math>I_c\,\!</math> is the half intensity point
- <math>n\,\!</math> is the refractive index of the polymer
and
- <math>V_{poly}= V_{ACtot} \frac {d_{poly}} {d_{poly} + d_{clad}} \cdot \sqrt {\frac {\epsilon_{clad}} {\epsilon _{poly}}}\,\!</math>
The measured quanitities are:
- <math>I= 2I_M\,\!</math> Modulated Intensity
- <math>I_0 = 2I_C\,\!</math> Output intensity
- <math>V_m = V_0 sin\omega t\,\!</math> Modulation Voltage
Teng_Mann techniques allows real-time optimization of processing conditions because you can evaluate r33 during the poling process. It is used to confirm that a sample has been poled. The R33 measurement is best used as a relative measure because it can be inaccurate. Use attenuated total reflection ATR to get an accurate absolute measure.
See Khanarian 1996 [2]
See STC-MDITR research project 1.1 [3]
Technique
video to come
Significance
References
- ↑ http://en.wikipedia.org/wiki/Ellipsometry
- ↑ Khanarian, et. al., JOSA B13, 1927 (1996)
- ↑ http://stc-mditr.org/research/oeoaomd/projects/1.111.cfm Measuring R33 with Interferometry