stokes polarimetry
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2021 ◽  
Author(s):  
Mariia Borovkova ◽  
Oleksii Sieryi ◽  
Jens Pahnke ◽  
Alexander Bykov ◽  
Igor Meglinski
Keyword(s):  

2021 ◽  
Vol 9 ◽  
Author(s):  
Vipin Tiwari ◽  
Yukti Pandey ◽  
Nandan S. Bisht

Mueller–Stokes polarimetry is emerging as a prominent noninvasive imaging technique to study the structural characteristics of an anisotropic medium. Spatial light modulator (SLM) is a programmable liquid crystal device (LCD), which is used to modulate the amplitude, phase, and polarization of light. The compact design and cumbrous manufacturing process of SLM requires its polarimetric calibration prior to its utilization for various applications. In this study, we experimentally demonstrate Mueller–Stokes imaging of a reflective-type SLM (Holoeye, LCR-720) to calibrate its polarization modulation characteristics with respect to its dynamic gray value range (0–255) at different spatial locations of SLM screen. Mueller matrices at 18 different gray values of SLM at an interval of 15, that is, at gray values 0, 15, 30, up to 255 have been experimentally measured using an improvised Mueller matrix imaging polarimeter (MMIP). Crucial polarimetric characteristics, that is, diattenuation, polarizance, state of polarization (SOP), depolarization, and retardance have been estimated with respect to the gray value range of SLM. Significant polarization modulation characteristics [diattenuation (0.08–0.3), polarizance (0.02–0.2), and retardance (0 to π)] have been determined for the SLM. These results indicate that the SLM exhibits spatially variable depolarizing nature and hence it is not perfectly homogeneous in structure. Therefore, it is expected that the outcomes of this study would be helpful for exploring the applicability of Mueller–Stokes polarimetry in advancement of LC technology.


Author(s):  
Andrés Márquez ◽  
Francisco J. Martínez-Guardiola ◽  
Marta Morales-Vidal ◽  
Daniel Puerto Garcia ◽  
Jorge Francés ◽  
...  

2021 ◽  
Vol 118 (5) ◽  
pp. 051104
Author(s):  
Saba N. Khan ◽  
Stuti Joshi ◽  
Bhaskar Kanseri ◽  
P. Senthilkumaran

Author(s):  
Mariia Borovkova ◽  
Oleksii Sieryi ◽  
Ivan Lopushenko ◽  
Natalia Kartashkina ◽  
Jens Pahnke ◽  
...  

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Gauri Arora ◽  
S. Deepa ◽  
Saba N. Khan ◽  
P. Senthilkumaran

AbstractStokes phase is the phase difference between orthogonal component states in the decomposition of any polarization state. Phase singularities in the Stokes phase distribution are Stokes singularities of an inhomogeneous polarization distribution. Under circular decomposition, Stokes phase distribution $$(\phi _{12})$$ ( ϕ 12 ) represents polarization azimuth $$(\gamma )$$ ( γ ) distribution and the singularities present in it are polarization singularities. Therefore, the charge of the Stokes vortices depicted as Stokes index $$\sigma _{12}$$ σ 12 is an important parameter associated with the polarization singularity. The Hybrid order Poincaré sphere (HyOPS)/Higher order Poincaré sphere (HOPS) beams, all having same Stokes index, contain a Stokes singularity at the center of the beam as these beams are constructed by vortex superposition. These beams, being superposition of orthogonal orbital angular momentum (OAM) states in orthogonal spin angular momentum (SAM) states can offer great multiplexing capabilities in communication. In this article, we identify these degenerate Stokes index states and discuss the ways and means of lifting this degeneracy. Otherwise, there are limitations on intensity based detection techniques, where demultiplexing or segregation of different HOPS/HyOPS beams is warranted. The method adduced here uses the diffraction of these beams through an equilateral triangular aperture in combination with polarization transformation as a probe to lift the Stokes index/Stokes phase degeneracy. Successively, the novelty of the detection scheme is discussed in the context of beams with alike polarization distributions where even the technique of Stokes polarimetry fails to predict the OAM and SAM content of the beam.


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