• Chinese Optics Letters
  • Vol. 18, Issue 9, 091404 (2020)
Y. F. Chen*, C. C. Lee, C. H. Wang, and M. X. Hsieh
Author Affiliations
  • Department of Electrophysics, Chiao Tung University, Hsinchu 30010
  • show less
    DOI: 10.3788/COL202018.091404 Cite this Article Set citation alerts
    Y. F. Chen, C. C. Lee, C. H. Wang, M. X. Hsieh. Laser transverse modes of spherical resonators: a review [Invited][J]. Chinese Optics Letters, 2020, 18(9): 091404 Copy Citation Text show less

    Abstract

    The study of structured laser beams has been one of the most active fields of research for decades, particularly in exploring laser beams with orbital angular momentum. The direct generation of structured beams from laser resonators is deeply associated with the formation of transverse modes. The wave representations of transverse modes of spherical cavities are usually categorized into Hermite–Gaussian (HG) and Laguerre–Gaussian (LG) modes for a long time. Enormous experimental results have revealed that the generalized representation for the transverse modes is the Hermite–LG (HLG) modes. We make a detailed overview for the theoretical description of the HLG modes from the representation of the spectral unitary group of order 2 in the Jordan–Schwinger map. Furthermore, we overview how to derive the integral formula for the elliptical modes based on the Gaussian wave-packet state and the inverse Fourier transform. The relationship between the HLG modes and elliptical modes is linked by the quantum Fourier transform. The most striking result is that the HLG modes can be exactly derived as the superposition of the elliptical modes without involving Hermite and Laguerre polynomials. Finally, we discuss the application of the HLG modes in characterizing the propagation evolution of the vortex structures of HG beams transformed by an astigmatic mode converter. This overview certainly provides not only a novel formula for transverse modes, but also a pedagogical insight into quantum physics.

    The quantum harmonic oscillator is an indispensable paradigm to understand the concept of quantum-classical correspondence, quantized radiation fields, and quantum optics. The eigenmodes of the two-dimensional (2D) quantum harmonic oscillator can be analytically solved as Hermite–Gaussian (HG) modes with rectangular symmetry or Laguerre–Gaussian (LG) modes with circular symmetry[1]. Since the paraxial wave equation for the spherical laser cavity is identical to the Schrödinger equation for the 2D harmonic oscillator, the HG and LG eigenmodes play an important role in exploring the laser transverse modes[24]. With the advent of end-pumped configurations, the high-order HG modes[58] and LG modes[915] can be efficiently generated in diode-pumped solid-state lasers. The Ince–Gaussian (IG) modes, another form of eigenfunctions to the paraxial wave equation, have been recently introduced[16] and been also experimentally observed in stable resonators[1719].

    References

    Y. F. Chen, C. C. Lee, C. H. Wang, M. X. Hsieh. Laser transverse modes of spherical resonators: a review [Invited][J]. Chinese Optics Letters, 2020, 18(9): 091404
    Download Citation