Paraxial and nonparaxial polynomial beams and the analytic approach to propagation
arXiv:1108.5906 · doi:10.1364/OL.36.004452
Abstract
We construct solutions of the paraxial and Helmholtz equations which are polynomials in their spatial variables. These are derived explicitly using the angular spectrum method and generating functions. Paraxial polynomials have the form of homogeneous Hermite and Laguerre polynomials in Cartesian and cylindrical coordinates respectively, analogous to heat polynomials for the diffusion equation. Nonparaxial polynomials are found by substituting monomials in the propagation variable with reverse Bessel polynomials. These explicit analytic forms give insight into the mathematical structure of paraxially and nonparaxially propagating beams, especially in regards to the divergence of nonparaxial analogs to familiar paraxial beams.
arXiv comment3 pages, Optics Letters style
Cited by in corpus (11)
- Particle-like topologies in light
- Singular knot bundle in light
- Knotted fields and explicit fibrations for lemniscate knots
- Propagation-invariant beams with quantum pendulum spectra: from Bessel beams to Gaussian beam-beams
- Generalized Bessel beams with two indices
- Fundamental Laser Modes in Paraxial Optics: From Computer Algebra and Simulations to Experimental Observation
- Excitation of knotted vortex lines in matter waves
- Constructing a polynomial whose nodal set is the three-twist knot
- Nodal-line dynamics via exact polynomial solutions for coherent waves traversing aberrated imaging systems
- Determinantal polynomial wave functions induced by random matrices
- Simple wave-optical superpositions as prime number sieves