Coherent-perfect-absorber and laser for bound states in a continuum
arXiv:1711.01986 · doi:10.1364/OL.43.000607
Abstract
It is shown that two fundamentally different phenomena, the bound states in continuum and the spectral singularity (or time-reversed spectral singularity), can occur simultaneously. This can be achieved, in particular, in a rectangular core dielectric waveguide with embedded active (or absorbing) layer. In such a system a two-dimensional bound state in a continuum is created in the plane of a waveguide cross section and it is emitted or absorbed along the waveguide core. The idea can be used for experimental implementation of a laser or a coherent-perfect-absorber for photonic bound state that resides in a continuous spectrum.
References in corpus (4)
- Coherent Perfect Absorbers: Time-reversed Lasers
- Anisotropy-induced photonic bound states in the continuum
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Cited by in corpus (14)
- Bound states in the continuum in photonic structures
- Topological properties of bound-states-in-the-continuum in geometries with broken anisotropy-symmetry
- Angular Control of Anisotropy-Induced Bound States in the Continuum
- Rabi oscillations of bound states in the continuum
- Ultra-sensitive Light Confinement Driven by Multiple Bound States in the Continuum
- Fate of Two-Particle Bound States in the Continuum in non-Hermitian Systems
- Spectral singularities and tunable slab lasers with 2D material coating
- Solvable model of bound states in the continuum (BIC) in one dimension
- Solving scattering problems in the half-line using methods developed for scattering in the full line
- Engineering bound states in continuum via nonlinearity induced extra dimension
- Solitary Spectrally-Discrete Bound States in the Continuum in an Open System
- Trapping wave fields in an expulsive potential by means of linear coupling
- Nonlinear dynamics of wave packets in tunnel-coupled harmonic-oscillator traps
- Dispersive bands of bound states in the continuum