Direct observation of the Faraday rotation using radially-polarised doughnut modes

TY - JOUR

T1 - Direct observation of the Faraday rotation using radially-polarised doughnut modes

AU - Tambag, F.

AU - Koksal, K.

AU - Yildiz, F.

AU - Babiker, M.

N1 - Funding Information: K.K and F.T. wish to thank Bitlis Eren University, Turkey for financial support (under the project: BEBAP 2021.02 ). Publisher Copyright: © 2023 Elsevier B.V.

PY - 2023/10/15

Y1 - 2023/10/15

N2 - A novel experimental technique for the realisation of the optical Faraday effect using Laguerre–Gaussian (LG) light is described. The experiment employs a zero-order vortex half-wave retarder to generate a radially or azimuthally-polarised LG doughnut beam. The light emerging from the retarder then passes through a linear polariser, which gives rise to two intensity lobes, with the orientation of the intensity gap between the two lobes pointing parallel (perpendicular) to the polarisation direction of the radially (azimuthally) polarised beam. To complete the Faraday set up, the light traverses a material subject to a magnetic field, before passing through a final linear polariser, which results in a visible rotation of the lobes pattern. This technique exhibits the Faraday effect readily visually, without further elaborate steps to detect changes in the light intensity. The degree of rotation of the plane of polarisation is determined directly by the visibly clear change in the orientation of the intensity gap between the lobes.

AB - A novel experimental technique for the realisation of the optical Faraday effect using Laguerre–Gaussian (LG) light is described. The experiment employs a zero-order vortex half-wave retarder to generate a radially or azimuthally-polarised LG doughnut beam. The light emerging from the retarder then passes through a linear polariser, which gives rise to two intensity lobes, with the orientation of the intensity gap between the two lobes pointing parallel (perpendicular) to the polarisation direction of the radially (azimuthally) polarised beam. To complete the Faraday set up, the light traverses a material subject to a magnetic field, before passing through a final linear polariser, which results in a visible rotation of the lobes pattern. This technique exhibits the Faraday effect readily visually, without further elaborate steps to detect changes in the light intensity. The degree of rotation of the plane of polarisation is determined directly by the visibly clear change in the orientation of the intensity gap between the lobes.

KW - Optical Faraday rotation

KW - Radial polarisation

KW - Twisted light

UR - http://www.scopus.com/inward/record.url?scp=85162015454&partnerID=8YFLogxK

U2 - 10.1016/j.optcom.2023.129649

DO - 10.1016/j.optcom.2023.129649

M3 - Article

AN - SCOPUS:85162015454

SN - 0030-4018

VL - 545

JO - Optics Communications

JF - Optics Communications

M1 - 129649

ER -