What, exactly, is a bound state in the continuum (BIC)? A BIC is an unconventional state that remains localized even upon its coexistence with the continuum of radiating modes. In theory, a BIC is characterized by the infinite radiative quality factor and zero linewidth.¹ Amongst the various types of BICs, the so-called Friedrich–Wintgen BIC arises due to the destructive interference of two resonances coupled to the same radiation channel. Once the eigenvalue of one of the resonances becomes purely real, the state turns into a BIC. Generally, Friedrich–Wintgen BICs lie in the vicinity of the frequency crossings of the uncoupled resonances.

Recently, the exploration of BICs in the strong coupling regime has gained increasing attention to diverse systems such as coupled photonic-plasmonic devices,² 2D materials,³ and low-contrast dielectric gratings.⁴ In some of these systems, strong coupling between resonances of different origin has been studied such as the interaction of plasmonic modes and the optical waveguide modes of a hybrid system² or the coupling of excitons and polaritons in a photonic crystal coupled to WSe2 monolayers.³ Such heterogeneous systems offer great opportunities for realizing new hybrid quasiparticles with rich physics. The Friedrich–Wintgen BICs arising in the vicinity of the avoided crossing of the resonance lead to very high-quality resonances.

In this issue of Advanced Photonics, Bogdanov et al.⁵ reveal the formation of the Friedrich–Wintgen BICs in a tiny resonant system as small as a nanoparticle (see Figure). First, the authors explore quasi-BIC states that arise due to the strong coupling between two classical phenomena (Mie-like and Fabry–Perot-like modes) supported by such a resonator. They then demonstrate that surprisingly high quality factors and strong light localization can be supported by a subwavelength cylinder due to the excitation of the quasi-BIC state. They also analytically examine the curious, tight relationship between the existence of the quasi-BIC states and the peculiarities of the Fano asymmetry parameter in the strong coupling regime, showing that the Fano asymmetry parameter becomes singular at the quasi-BIC point. The team confirmed this unusual strong coupling experimentally. By measuring the scattering cross-section of a cylindrical resonator filled with water, the authors are able to capture the “avoided crossing” (a direct confirmation of the case of strong coupling⁶) as a function of the cylinder aspect ratio.

The innovative ideas proposed and experimentally demonstrated by Bogdanov et al. could serve as a new paradigm for rapidly projecting the nascent BIC methodology onto numerous optical phenomena and applications that rely on high field localization and high quality factors, which now can be achieved with a single-particle resonator at the subwavelength scale, something that was difficult to achieve previously. On-a-chip applications such as low-threshold lasing and high-harmonic generation are examples of the many possibilities that would make use of such an exciting ultracompact novel nanophotonic platform.