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.
- Sep 11 2014 : Optica Research - Perfect Focus through Thick Layers May Bring Better Vision to Medicine
- Aug 28 2014 : Biomedical Optics Express Research - This is Your Brain's Blood Vessels on Drugs
- Aug 20 2014 : Optica Research - UAlberta Engineers Take Major Step Toward Photonic Circuits. Nano-optical cables could replace copper wiring on computer chips… more
- Aug 06 2014 : Optica Research - New Hand-Held Device Uses Lasers, Sound Waves for Deeper Melanoma Imaging
- 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...