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Chapter 7:
Optical Vortices
Editor(s): Mikhail A. Noginov; Graeme Dewar; Martin W. McCall; Nikolay I. Zheludev
Author(s): Dennis, Mark R.; Padgett, Miles J.; O'Holleran, Kevin
Published: 2009
DOI: 10.1117/3.832717.ch7
To fully describe even a monochromatic light field, one needs to specify its magnitude, phase, and polarization state, all as a function of spatial position. The requirement to specify the polarization is commensurate with the light being a vector field. However, in many optical systems and associated phenomena, the polarization is uniform throughout the field, and it is sufficient to consider the light as a scalar field with only its magnitude and phase being spatially dependent. In such systems, if one examines any cross-section through the complicated light field, one aspect of the light's phase distribution is immediately apparent. Throughout the cross-section there are positions of phase singularity where all phases meet, and around which the phase changes by 2π, in either a clockwise or anticlockwise direction.
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