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Quasibound states in the continuum in photonic-crystal-based optomechanical microcavities
Optics · Submitted 30 Jun 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that a suspended photonic-crystal slab facing a distributed Bragg reflector realizes an optomechanical system with a quasi-bound state in the continuum.
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The abstract, sentence by sentence
We present a detailed study of mechanically compliant, photonic-crystal-based microcavities featuring a quasi-bound state in the continuum. Such systems have recently been predicted to reduce the optical loss in Fabry-Perot-type optomechanical cavities. However, they require two identical photonic-crystal slabs facing each other, which poses a considerable challenge for experimental implementation. We investigate how such an ideal system can be simplified and still exhibit a quasi-bound state in the continuum. We find that a suspended photonic-crystal slab facing a distributed Bragg reflector realizes an optomechanical system with a quasi-bound state in the continuum. In this system, the radiative cavity loss can be eliminated to the extent that the cavity loss is dominated by dissipative loss originating from material absorption only. These proposed optomechanical cavity designs are predicted to feature optical quality factors in excess of 10^5.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a detailed study of mechanically compliant, photonic-crystal-based microcavities featuring a quasi-bound state in the continuum. | contribution 1.00 | 0.87 | 0.08 | asserted 0.99 |
| s1 | Such systems have recently been predicted to reduce the optical loss in Fabry-Perot-type optomechanical cavities. | background 1.00 | 0.03 | 0.03 | hedged possibility 0.57 |
| s2 | However, they require two identical photonic-crystal slabs facing each other, which poses a considerable challenge for experimental implementation. | background 0.67 | 0.07 | 0.03 | asserted 1.00 |
| s3 | We investigate how such an ideal system can be simplified and still exhibit a quasi-bound state in the continuum. | contribution 0.91 | 0.51 | 0.05 | unclear 0.60 |
| s4 | We find that a suspended photonic-crystal slab facing a distributed Bragg reflector realizes an optomechanical system with a quasi-bound state in the continuum. | result 0.68 | 0.92 | 0.67 | asserted 1.00 |
| s5 | In this system, the radiative cavity loss can be eliminated to the extent that the cavity loss is dominated by dissipative loss originating from material absorption only. | result 0.97 | 0.72 | 0.32 | asserted 0.89 |
| s6 | These proposed optomechanical cavity designs are predicted to feature optical quality factors in excess of 10^5. | result 0.98 | 0.59 | 0.29 | hedged possibility 0.86 |
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Original abstract
We present a detailed study of mechanically compliant, photonic-crystal-based microcavities featuring a quasi-bound state in the continuum. Such systems have recently been predicted to reduce the optical loss in Fabry-Perot-type optomechanical cavities. However, they require two identical photonic-crystal slabs facing each other, which poses a considerable challenge for experimental implementation. We investigate how such an ideal system can be simplified and still exhibit a quasi-bound state in the continuum. We find that a suspended photonic-crystal slab facing a distributed Bragg reflector realizes an optomechanical system with a quasi-bound state in the continuum. In this system, the radiative cavity loss can be eliminated to the extent that the cavity loss is dominated by dissipative loss originating from material absorption only. These proposed optomechanical cavity designs are predicted to feature optical quality factors in excess of 10^5.
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1 arXiv paper cite this in 3 sentences
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When using such PhC membranes as an end-mirror [ref] in our proposed microcavity, an optomechanical frequency pulling factor of about $2π·100$GHz/nm would be realized leading to a single-photon coupling strength on the order of $2π·500$kHz and a ratio of coupling strength to optical loss of $g_0/κ∼5·10^-3$, which is comparable to realizations based on optomechanical crystals [ref] , microwave optomechanics [ref] , or magnetomechanics [ref] .
Cavity optomechanical bistability with an ultrahigh reflectivity photonic crystal membrane · Conclusion · 0.93
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