Abstract
The capability of optical resonators to extend the effective radiation-matter interaction length originates from a multipass effect, hence is intrinsically limited by the resonator’s quality factor. Here, we show that this constraint can be overcome by combining the concepts of resonant interaction and coherent perfect absorption (CPA). We demonstrate and investigate super-resonant coherent absorption in a coupled Fabry-Perot (FP)/ring cavity structure. At the FP resonant wavelengths, the described phenomenon gives rise to split modes with a nearly-transparent peak and a peak whose transmission is exceptionally sensitive to the intracavity loss. For small losses, the effective interaction pathlength of these modes is proportional respectively to the ratio and the product of the individual finesse coefficients of the two resonators. The results presented extend the conventional definition of resonant absorption and point to a way of circumventing the technological limitations of ultrahigh-quality resonators in spectroscopy and optical sensing schemes.
Highlights
The capability of optical resonators to extend the effective radiation-matter interaction length originates from a multipass effect, is intrinsically limited by the resonator’s quality factor. We show that this constraint can be overcome by combining the concepts of resonant interaction and coherent perfect absorption (CPA)
The results presented extend the conventional definition of resonant absorption and point to a way of circumventing the technological limitations of ultrahighquality resonators in spectroscopy and optical sensing schemes
We show that the CPA features can be combined with the resonant enhancement of a conventional ring cavity to achieve an exceptional sensitivity to the intracavity loss
Summary
The capability of optical resonators to extend the effective radiation-matter interaction length originates from a multipass effect, is intrinsically limited by the resonator’s quality factor. Since the perfect extinction of the input field stems from a very critical balance of interference and dissipation, the transmission of a coherent absorber when approaching the CPA condition is very sensitive to small variations of the intracavity loss.
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