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Questions related to the beam path length are resolved.
The nanofluid is held in quartz cuvettes, with 10 mm beam path length.
Individual foci in the propagated beam path are not separable any more.
Each powder sample was sandwiched between two pieces of KAPTON tape located on the beam path.
Figure 5 Internal displacement field and simulated beam path within SiGe DMs.
Averaged temperature across the entire light beam path inside the slab vs. time.
The central stripe is the 0 order indicating the refracted beam path.
A first lens on the laser beam path is used to compensate for the beam divergence.
The change in refractive index due to heat concentrated in one spot along the beam path is equivalent to the change due to heat distributed along the entire beam path.
However, as discussed previously for XRF studies, the controlled thickness of thin-sections may limit averaging effect along beam path.
The beam path is represented by the weighting values w n as shown for the twofold DM in Figure 5b.
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