Topics in this Issue
Part (a) shows the intensity distribution of a laser beam diffracted from the currently read microhologram, while part (b) shows the same beam focused on the detector. Its detected power is the signal. Parts (c) and (d) are the same intensity distributions for one of the many thousands of other microholograms recorded into the material. For further details, see the paper by Nagy et al., pp. 753-761.
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- Optical properties of the metals Al, Co, Cu, Au, Fe, Pb,...
- Optical properties of metallic films for vertical-cavity...
- Phase retrieval algorithms: a comparison
- Laser Beams and Resonators
- Recent advances in digital holography [Invited]
- Measuring very low optical powers with a common camera
- Exact analytic solutions of Maxwell’s equations...
- Simplifying numerical ray tracing for characterization of...
- Optical Constants of Water in the 200-nm to 200-?m...
- Multimode interference devices with...