Abstract
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We have developed an interferometric optical reflectivity microscope to observe the phase-sensitive reflectivity of nanophotonic structures with high spatial and spectral resolution over broad frequency ranges from 4000 to 13300 cm-1, corresponding to wavelengths 750 < λ < 2500 nm. From the frequency-resolved phases we obtain the (group) time delay. We study planar microcavities made from GaAs/AlAs, and three-dimensional (3D) photonic band gap crystals made from silicon with the woodpile structure. Measurements on planar microcavities have been compared with analytic transfer matrix theory, where an excellent agreement is found. The mean difference between measured and calculated reflectivity is better than 4 percent-points. For a planar microcavity with a stopband centred at 1331 nm and a relative bandwidth of 16% we observe time delays exceeding 4 ps at the edge of the stopband. For the 3D woodpile structure we observe time delays exceeding 550 fs at the edge of the 3D bandgap. Combined with the very thin metasurface like structure, this yields a lower bound for the group index of n_g≥210, much more than previously observed in photonic crystal waveguides. Current studies include developing a model for the 3D woodpile crystal to understand the large group delay.
We have developed an interferometric optical reflectivity microscope to observe the phase-sensitive reflectivity of nanophotonic structures with high spatial and spectral resolution over broad frequency ranges from 4000 to 13300 cm-1, corresponding to wavelengths 750 < λ < 2500 nm. From the frequency-resolved phases we obtain the (group) time delay. We study planar microcavities made from GaAs/AlAs, and three-dimensional (3D) photonic band gap crystals made from silicon with the woodpile structure. Measurements on planar microcavities have been compared with analytic transfer matrix theory, where an excellent agreement is found. The mean difference between measured and calculated reflectivity is better than 4 percent-points. For a planar microcavity with a stopband centred at 1331 nm and a relative bandwidth of 16% we observe time delays exceeding 4 ps at the edge of the stopband. For the 3D woodpile structure we observe time delays exceeding 550 fs at the edge of the 3D bandgap. Combined with the very thin metasurface like structure, this yields a lower bound for the group index of n_g≥210, much more than previously observed in photonic crystal waveguides. Current studies include developing a model for the 3D woodpile crystal to understand the large group delay.
| Original language | English |
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| Publication status | Published - 2 Dec 2024 |
| Event | GdR Complexe Annual Meeting 2024 - Paris, France Duration: 2 Dec 2024 → 4 Dec 2024 |
Workshop
| Workshop | GdR Complexe Annual Meeting 2024 |
|---|---|
| Country/Territory | France |
| City | Paris |
| Period | 2/12/24 → 4/12/24 |
Keywords
- Group delay
- photonic crystal
- interferometry
- broadband
- metasurface