Analysis of a segmented q-plate tunable retarder for the generation of first-order vector beams.

In this work we study a prototype q-plate segmented tunable liquid crystal retarder device. It shows a large modulation range (5π rad for a wavelength of 633 nm and near 2π for 1550 nm) and a large clear aperture of one inch diameter. We analyze the operation of the q-plate in terms of Jones matrices and provide different matrix decompositions useful for its analysis, including the polarization transformations, the effect of the tunable phase shift, and the effect of quantization levels (the device is segmented in 12 angular sectors). We also show a very simple and robust optical system capable of generating all polarization states on the first-order Poincaré sphere. An optical polarization rotator and a linear retarder are used in a geometry that allows the generation of all states in the zero-order Poincaré sphere simply by tuning two retardance parameters. We then use this system with the q-plate device to directly map an input arbitrary state of polarization to a corresponding first-order vectorial beam. This optical system would be more practical for high speed and programmable generation of vector beams than other systems reported so far. Experimental results are presented.

[1]  Enrico Santamato,et al.  Photon spin-to-orbital angular momentum conversion via an electrically tunable q-plate , 2010, 1010.4473.

[2]  L. Marrucci,et al.  Pancharatnam-Berry phase optical elements for wave front shaping in the visible domain: Switchable helical mode generation , 2006, 0712.0101.

[3]  Kateryna Kushnir,et al.  Q-plates micro-arrays for parallel processing of the photon orbital angular momentum , 2014 .

[4]  Chun-qing Gao,et al.  Generation of optical vortices by using spiral phase plates made of polarization dependent devices. , 2014, Optics letters.

[5]  M. Padgett,et al.  Orbital angular momentum: origins, behavior and applications , 2011 .

[6]  A. Willner,et al.  4 × 20  Gbit/s mode division multiplexing over free space using vector modes and a q-plate mode (de)multiplexer. , 2014, Optics letters.

[7]  Q. Zhan Cylindrical vector beams: from mathematical concepts to applications , 2009 .

[8]  Enrico Santamato,et al.  Tunable liquid crystal q-plates with arbitrary topological charge. , 2011, Optics express.

[9]  Enrico Santamato,et al.  Liquid crystal spatial-mode converters for the orbital angular momentum of light , 2012, 1209.4534.

[10]  Jeffrey A. Davis,et al.  Analysis of multilevel spiral phase plates using a Dammann vortex sensing grating. , 2010, Optics express.

[11]  Jianping Ding,et al.  Optimal phase steps of multi-level spiral phase plates , 2006 .

[12]  J. Davis,et al.  Two-dimensional polarization encoding with a phase-only liquid-crystal spatial light modulator. , 2000, Applied optics.

[13]  Gerd Leuchs,et al.  Classical and quantum properties of cylindrically polarized states of light. , 2010, Optics express.

[14]  R. R. Alfano,et al.  Cylindrical vector beam generation from a multi elliptical core optical fiber , 2011, CLEO: 2011 - Laser Science to Photonic Applications.

[15]  Peter G. Kazansky,et al.  Radially polarized optical vortex converter created by femtosecond laser nanostructuring of glass , 2011 .

[16]  Nelson Tabiryan,et al.  Fabrication of liquid crystal polymer axial waveplates for UV-IR wavelengths. , 2009, Optics express.

[17]  M Stalder,et al.  Linearly polarized light with axial symmetry generated by liquid-crystal polarization converters. , 1996, Optics letters.

[18]  Jorge Albero,et al.  Polarization manipulation of radially polarized beams , 2012 .

[19]  Shuangchun Wen,et al.  Realization of polarization evolution on higher-order Poincaré sphere with metasurface , 2014, 1407.1997.

[20]  Erez Hasman,et al.  Topological spin-orbit interaction of light in anisotropic inhomogeneous subwavelength structures. , 2008, Optics letters.

[21]  Chun Ye,et al.  Construction of an optical rotator using quarter-wave plates and an optical retarder , 1995 .

[22]  Ebrahim Karimi,et al.  Efficient generation and sorting of orbital angular momentum eigenmodes of light by thermally tuned q-plates , 2009, 0905.0562.

[23]  R. Alfano,et al.  Measuring the self-healing of the spatially inhomogeneous states of polarization of vector Bessel beams , 2015 .

[24]  C. Fernández-Pousa,et al.  Polarizing diffraction-grating triplicators. , 2001, Optics letters.

[25]  Jun Amako,et al.  Transmission variations in liquid crystal spatial light modulators caused by interference and diffraction effects , 1999 .

[26]  Shuangchun Wen,et al.  Generation of arbitrary cylindrical vector beams on the higher order Poincaré sphere. , 2014, Optics letters.

[27]  D. Nolan,et al.  Higher-order Poincaré sphere, stokes parameters, and the angular momentum of light. , 2011, Physical review letters.

[28]  Jeffrey A. Davis,et al.  Encoding high-order cylindrically polarized light beams. , 2014, Applied optics.

[29]  G Leuchs,et al.  Sharper focus for a radially polarized light beam. , 2003, Physical review letters.

[30]  L. Marrucci,et al.  Optical spin-to-orbital angular momentum conversion in inhomogeneous anisotropic media. , 2006, Physical review letters.

[31]  Ebrahim Karimi,et al.  Polarization-controlled evolution of light transverse modes and associated Pancharatnam geometric phase in orbital angular momentum , 2010 .

[32]  D. Fan,et al.  Hybrid-order Poincare sphere , 2014, 1411.2476.

[33]  Gerd Leuchs,et al.  Focusing light to a tighter spot , 2000 .