Difference between revisions of "Second-order Material Characterization"
Jump to navigation
Jump to search
Cmditradmin (talk | contribs) |
Cmditradmin (talk | contribs) |
||
Line 11: | Line 11: | ||
β, the first nonlinear polarizability depends on molecular structure, environment and measurement frequency. There are several tools that help us characterize the materials. | β, the first nonlinear polarizability depends on molecular structure, environment and measurement frequency. There are several tools that help us characterize the materials. | ||
[[Hyper Rayleigh Scattering]] | [[Hyper Rayleigh Scattering]] | ||
[[Teng-Mann Method] | |||
[[ | [[Attenuated_Total_Reflectance]] | ||
[[category:second order NLO]] | [[category:second order NLO]] | ||
<table id="toc" style="width: 100%"> | <table id="toc" style="width: 100%"> |
Revision as of 10:01, 9 August 2010
Previous Topic | Return to Second-order Processes, Materials & Characterization Menu |
Characterization
β, the first nonlinear polarizability depends on molecular structure, environment and measurement frequency. There are several tools that help us characterize the materials.
[[Teng-Mann Method]
Previous Topic | Return to Second-order Processes, Materials & Characterization Menu |