Pancharatnam lens acts as improved diffractive lens

Nov. 13, 2015
A group has made an ultrathin (2.26 μm) f/2.1 Pancharatnam lens using a polarization holography alignment technique.
Content Dam Lfw Print Articles 2015 11 1511lfw Nb F2

In a "Pancharatnam" phase-modifying optical device, the polarization state of a circularly polarized wavefront passing through the device is modified by the device as a continuous function of the position across the device. For example, a Pancharatnam lens is basically a half-wave retarder, with the retarder's local optical axis aligned with the azimuthal angle at that point. Such a lens—when designed as a positive lens for, say, right-handed, circularly polarized light—focuses light as a positive lens should, but becomes a negative lens when left-handed circularly polarized light is passed through the lens. Pancharatnam lenses have previously been fabricated by microrubbing, creating a space-variant subwavelength dielectric grating, or via holographic alignment. Now, a group at Kent State University (Kent, OH) has made an ultrathin (2.26 μm) f/2.1 Pancharatnam lens using a polarization holography alignment technique. The technique, which is low-cost, could be applicable to a wide size range.

Unlike a conventional diffractive lens, a Pancharatnam lens does not diffract light into undesired orders. However, like ordinary diffractive lenses, it does have a strong wavelength dependence. The researchers fabricated an experimental device for a 632 nm wavelength using a photoalignment layer that shows a strong orientational response to the local polarization axis of light, and is exposed in a holographic setup to provide the desired half-wave retarder orientation. The result is a polarization axis that is a function of the radial distance from the center of the pattern with a gradually decreased grating pitch to the edge. The design of the fabricated device had a parabolic phase profile and showed the expected imaging properties, which were good imaging quality for low f numbers and some degradation for higher f numbers. A design modeling the optimal diffraction-limited asphere would avoid the image degradation. Reference: K. Gao et al., Opt. Express, 23, 20, 26086 (Oct. 5, 2015).

About the Author

John Wallace | Senior Technical Editor (1998-2022)

John Wallace was with Laser Focus World for nearly 25 years, retiring in late June 2022. He obtained a bachelor's degree in mechanical engineering and physics at Rutgers University and a master's in optical engineering at the University of Rochester. Before becoming an editor, John worked as an engineer at RCA, Exxon, Eastman Kodak, and GCA Corporation.

Sponsored Recommendations

Brain Computer Interface (BCI) electrode manufacturing

Jan. 31, 2025
Learn how an industry-leading Brain Computer Interface Electrode (BCI) manufacturer used precision laser micromachining to produce high-density neural microelectrode arrays.

Electro-Optic Sensor and System Performance Verification with Motion Systems

Jan. 31, 2025
To learn how to use motion control equipment for electro-optic sensor testing, click here to read our whitepaper!

How nanopositioning helped achieve fusion ignition

Jan. 31, 2025
In December 2022, the Lawrence Livermore National Laboratory's National Ignition Facility (NIF) achieved fusion ignition. Learn how Aerotech nanopositioning contributed to this...

Nanometer Scale Industrial Automation for Optical Device Manufacturing

Jan. 31, 2025
In optical device manufacturing, choosing automation technologies at the R&D level that are also suitable for production environments is critical to bringing new devices to market...

Voice your opinion!

To join the conversation, and become an exclusive member of Laser Focus World, create an account today!