Advanced Photonics, Volume. 2, Issue 3, 036003(2020)

Transmission of vector vortex beams in dispersive media

Ilaria Gianani1,2, Alessia Suprano1, Taira Giordani1, Nicolò Spagnolo1, Fabio Sciarrino1,3、*, Dimitris Gorpas4,5, Vasilis Ntziachristos4,5, Katja Pinker6, Netanel Biton7, Judy Kupferman7, and Shlomi Arnon7
Author Affiliations
  • 1Sapienza Università di Roma, Dipartimento di Fisica, Rome, Italy
  • 2Università degli Studi Roma Tre, Dipartimento di Scienze, Rome, Italy
  • 3Consiglio Nazionale delle Ricerche, Istituto dei Sistemi Complessi, Roma, Italy
  • 4Technische Universität München, Biological Imaging and Center for Translational Cancer Research, Munich, Germany
  • 5Institute of Biological and Medical Imaging, Helmholtz Zentrum München, Neuherberg, Germany
  • 6Medical University of Vienna, Department of Biomedical Imaging and Image-Guided Therapy, Molecular and Gender Imaging Service, Vienna, Austria
  • 7Ben-Gurion University of the Negev, Department of Electrical and Computer Engineering, Beer Sheva, Israel
  • show less
    Figures & Tables(5)
    Experimental scheme. A CW laser emits a Gaussian beam with m=0, at 808 nm. Then, the preparation stage for the initial polarization state is made with a PBS, QWP, and HWP. Five units, each composed of a q-plate (oval blue symbol) followed by an HWP (pink rectangle), generate structured light. Our q-plates display a charge q=0.5, which increases (decreases) the OAM number by 1. In the inset, we report the optical axis orientation of the plate and the phase acquired by the wavefront in the transverse plane ϕ(x,y) conditionally to the polarization states (L,R). After this preparation stage, we obtain VVBs in the form of Eq. (2), shown in the second inset of the figure (H, horizontal polarization; V, vertical polarization; D, diagonal polarization; A, antidiagonal polarization; L, left circular polarization; and R, right circular polarization). Depending on the analysis, we can use the whole vectorial field or the scalar fields produced by a suitable projection of the polarization on the basis b. The second stage consists of the sample, prepared with several concentrations of latex beads, and the detection platform. An objective collects the scattered light and focuses the image on the CCD camera. A polarization analyzer can be inserted between the sample and the objective.
    Contrast analysis. (a) Recorded beam profiles associated with OAM 5 for three different concentrations C=0%, 0.10%, 0.12%. In each image, the red line indicates the selected slice for the fitting procedure. (b) Fit on the selected slices, for the same concentration of the above panel. Contrast ratio in a logarithmic scale for (c) circularly polarized OAM modes, (d) linearly and circularly polarized Gaussian modes, and (e) several VVBs modes as a function of the beads concentration, respectively.
    Depolarization analysis. (a) Pixel-by-pixel DR for the VVB mode with m1=5 and m2=−5, for three different concentrations C=0%, 0.10%, 0.12%. (b) Spatial profile of the same mode for comparison. (c) Pixel-by-pixel DR for a circularly polarized Gaussian mode, for three different concentrations C=0%, 0.10%, 0.12%. (d) Spatial profile of the same mode for comparison.
    Polarization pattern analysis. RGB map of the Stokes parameters for the VVB mode with m1=5 and m2=−5, for three different concentrations C=0%, 0.10%, 0.12%.
    • Table 1. Scattering properties of latex beads. The relevant parameters of our scattering samples are reported, namely the scattering length ls, transmission length ltr, scattering coefficient μs, the inverse of transmission length μs, the scattering anisotropic coefficient g, and the quantity μsL, where L=1  cm is the sample length. Those parameters are determined to provide a complete picture of the scattering conditions corresponding to the performed experimental tests. The values were retrieved for different concentrations C of latex beads. The calculations were obtained using the program available in Ref. 50.

      View table
      View in Article

      Table 1. Scattering properties of latex beads. The relevant parameters of our scattering samples are reported, namely the scattering length ls, transmission length ltr, scattering coefficient μs, the inverse of transmission length μs, the scattering anisotropic coefficient g, and the quantity μsL, where L=1  cm is the sample length. Those parameters are determined to provide a complete picture of the scattering conditions corresponding to the performed experimental tests. The values were retrieved for different concentrations C of latex beads. The calculations were obtained using the program available in Ref. 50.

      C (%)ls (μm)ltr (μm)μs=1/ls (cm1)μs=1/ltr (cm1)gμsL
      0.05150714,5276.630.690.8966.63
      0.08942907910.611.100.89610.61
      0.09838807011.191.240.89611.19
      0.10754726313.21.380.89613.2
      0.11686660314.61.510.89614.6
      0.12629605315.91.650.89615.9
    Tools

    Get Citation

    Copy Citation Text

    Ilaria Gianani, Alessia Suprano, Taira Giordani, Nicolò Spagnolo, Fabio Sciarrino, Dimitris Gorpas, Vasilis Ntziachristos, Katja Pinker, Netanel Biton, Judy Kupferman, Shlomi Arnon, "Transmission of vector vortex beams in dispersive media," Adv. Photon. 2, 036003 (2020)

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category: Research Articles

    Received: Feb. 14, 2020

    Accepted: May. 7, 2020

    Published Online: May. 22, 2020

    The Author Email: Sciarrino Fabio (fabio.sciarrino@uniroma1.it)

    DOI:10.1117/1.AP.2.3.036003

    Topics