Installation3
Installation 3: Optical transmission and reflectivity and light scattering
Optical transmission |
allowing optical absorption coefficient determination and imaginary part of refraction index |
Gas absorption (Samson cell): |
allowing gas optical absorption cross sections determination |
Optical reflectivity | allowing material optical reflectivity determination and providing entry data for determination of real and imaginary parts of dielectric constant (e.g. by Kramers-Kronig relations or fitting to the experiment) in cubic and anisotropic materials |
Light scattering |
providing entry data for roughness determination and optical slope errors |
How to measure:
Optical transmission |
Optical transmission and related absorption coefficient can be obtained in a variety of modes, incidence geometries and polarization state in the photon energy range covered by BABE including:
Codes for analysis of anisotropic materials transmission can be provided |
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Optical reflectivity |
Optical reflectivity and material optical constants can be obtained in a variety of modes, incidence geometries and polarization state in the photon energy range covered by BABE Detection of incident and reflected light can be accomplished by photodiodes or electron multiplier detectors |
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Light scattering |
Diffuse reflectivity – Light scattering provides access to surface roughness and slope errors in the photon energy range covered by BABE including rocking scan and detector scan modes with a typical wave vector resolution of the order of 10-2 nm-1
. Light detection is accomplished by photodiodes or electron multipliers, custom detection systems – e.g. by CCD detector – can be considered |