2010/11/16 by Chun-Fang Li, Xi Chen, Li, Chun-Fang +1
Chemistry · Physics and Astronomy · #Advanced Physical and Chemical Molecular Interactions #Atomic and Molecular Physics #FOS: Physical sciences #Optics (physics.optics) #Quantum Physics (quant-ph) #Quantum optics and atomic interactions #physics.optics #quant-ph
paper · pdf · doi:10.48550/arxiv.1011.3608
14 pages and 1 figure
arxiv created 2010/11/16 · openalex publication_date 2010/11/16 · arxiv updated 2010/11/17 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
Any polarization vector of a plane wave can be decomposed into a pair of mutually orthogonal base vectors, known as a polarization basis. Regarding this decomposition as a quasi-unitary transformation from a three-component vector to a corresponding two-component spinor, one is led to a representation formalism for the photon spin. The spin operator \boldsymbol γ defined on the space of unit spinors, referred to as the Jones space, has only component along the wave vector and is represented by one of the Pauli matrices in the commonly used polarization basis. It is deformed by the quasi-unitary transformation from the spin operator that is defined on the space of unit polarization vectors, referred to as the Pancharatnam space. On the basis of this theory, it is shown that the Cartesian components of spin operator \boldsymbol γ are mutually commutative and the spin angular momentum in units of ℏ is exactly the component of the Stokes vector along the wave vector.