Experimental probe of a complete 3D photonic band gap

Research output: Contribution to journalJournal articleResearchpeer-review

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Experimental probe of a complete 3D photonic band gap. / Adhikary, Manashee; Uppu, Ravitej; Harteveld, Cornelis A. M.; Grishina, Diana A.; Vos, Willem L.

In: Optics Express, Vol. 28, No. 3, 03.02.2020, p. 2683-2698.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Adhikary, M, Uppu, R, Harteveld, CAM, Grishina, DA & Vos, WL 2020, 'Experimental probe of a complete 3D photonic band gap', Optics Express, vol. 28, no. 3, pp. 2683-2698. https://doi.org/10.1364/OE.28.002683

APA

Adhikary, M., Uppu, R., Harteveld, C. A. M., Grishina, D. A., & Vos, W. L. (2020). Experimental probe of a complete 3D photonic band gap. Optics Express, 28(3), 2683-2698. https://doi.org/10.1364/OE.28.002683

Vancouver

Adhikary M, Uppu R, Harteveld CAM, Grishina DA, Vos WL. Experimental probe of a complete 3D photonic band gap. Optics Express. 2020 Feb 3;28(3):2683-2698. https://doi.org/10.1364/OE.28.002683

Author

Adhikary, Manashee ; Uppu, Ravitej ; Harteveld, Cornelis A. M. ; Grishina, Diana A. ; Vos, Willem L. / Experimental probe of a complete 3D photonic band gap. In: Optics Express. 2020 ; Vol. 28, No. 3. pp. 2683-2698.

Bibtex

@article{3070771931da4e9c96e307df44bd16ae,
title = "Experimental probe of a complete 3D photonic band gap",
abstract = "The identification of a complete three-dimensional (3D) photonic band gap in real crystals typically employs theoretical or numerical models that invoke idealized crystal structures. Such an approach is prone to false positives (gap wrongly assigned) or false negatives (gap missed). Therefore, we propose a purely experimental probe of the 3D photonic band gap that pertains to any class of photonic crystals. We collect reflectivity spectra with a large aperture on exemplary 3D inverse woodpile structures that consist of two perpendicular nanopore arrays etched in silicon. We observe intense reflectivity peaks (R>90%) typical of high-quality crystals with broad stopbands. A resulting parametric plot of s-polarized versus p-polarized stopband width is linear ({"}y=x{"}), a characteristic of a 3D photonic band gap, as confirmed by simulations. By scanning the focus across the crystal, we track the polarization-resolved stopbands versus the volume fraction of high-index material and obtain many more parametric data to confirm that the high-NA stopband corresponds to the photonic band gap. This practical probe is model-free and provides fast feedback on the advanced nanofabrication needed for 3D photonic crystals and stimulates practical applications of band gaps in 3D silicon nanophotonics and photonic integrated circuits, photovoltaics, cavity QED, and quantum information processing. (C) 2020 Optical Society of America under the terms of the OSA Open Access Publishing Agreement",
keywords = "SPONTANEOUS EMISSION, LIGHT-EMISSION, WAVE-GUIDES, CRYSTALS, DIFFRACTION, FABRICATION",
author = "Manashee Adhikary and Ravitej Uppu and Harteveld, {Cornelis A. M.} and Grishina, {Diana A.} and Vos, {Willem L.}",
note = "Hy Q",
year = "2020",
month = feb,
day = "3",
doi = "10.1364/OE.28.002683",
language = "English",
volume = "28",
pages = "2683--2698",
journal = "Optics Express",
issn = "1094-4087",
publisher = "The Optical Society",
number = "3",

}

RIS

TY - JOUR

T1 - Experimental probe of a complete 3D photonic band gap

AU - Adhikary, Manashee

AU - Uppu, Ravitej

AU - Harteveld, Cornelis A. M.

AU - Grishina, Diana A.

AU - Vos, Willem L.

N1 - Hy Q

PY - 2020/2/3

Y1 - 2020/2/3

N2 - The identification of a complete three-dimensional (3D) photonic band gap in real crystals typically employs theoretical or numerical models that invoke idealized crystal structures. Such an approach is prone to false positives (gap wrongly assigned) or false negatives (gap missed). Therefore, we propose a purely experimental probe of the 3D photonic band gap that pertains to any class of photonic crystals. We collect reflectivity spectra with a large aperture on exemplary 3D inverse woodpile structures that consist of two perpendicular nanopore arrays etched in silicon. We observe intense reflectivity peaks (R>90%) typical of high-quality crystals with broad stopbands. A resulting parametric plot of s-polarized versus p-polarized stopband width is linear ("y=x"), a characteristic of a 3D photonic band gap, as confirmed by simulations. By scanning the focus across the crystal, we track the polarization-resolved stopbands versus the volume fraction of high-index material and obtain many more parametric data to confirm that the high-NA stopband corresponds to the photonic band gap. This practical probe is model-free and provides fast feedback on the advanced nanofabrication needed for 3D photonic crystals and stimulates practical applications of band gaps in 3D silicon nanophotonics and photonic integrated circuits, photovoltaics, cavity QED, and quantum information processing. (C) 2020 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

AB - The identification of a complete three-dimensional (3D) photonic band gap in real crystals typically employs theoretical or numerical models that invoke idealized crystal structures. Such an approach is prone to false positives (gap wrongly assigned) or false negatives (gap missed). Therefore, we propose a purely experimental probe of the 3D photonic band gap that pertains to any class of photonic crystals. We collect reflectivity spectra with a large aperture on exemplary 3D inverse woodpile structures that consist of two perpendicular nanopore arrays etched in silicon. We observe intense reflectivity peaks (R>90%) typical of high-quality crystals with broad stopbands. A resulting parametric plot of s-polarized versus p-polarized stopband width is linear ("y=x"), a characteristic of a 3D photonic band gap, as confirmed by simulations. By scanning the focus across the crystal, we track the polarization-resolved stopbands versus the volume fraction of high-index material and obtain many more parametric data to confirm that the high-NA stopband corresponds to the photonic band gap. This practical probe is model-free and provides fast feedback on the advanced nanofabrication needed for 3D photonic crystals and stimulates practical applications of band gaps in 3D silicon nanophotonics and photonic integrated circuits, photovoltaics, cavity QED, and quantum information processing. (C) 2020 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

KW - SPONTANEOUS EMISSION

KW - LIGHT-EMISSION

KW - WAVE-GUIDES

KW - CRYSTALS

KW - DIFFRACTION

KW - FABRICATION

U2 - 10.1364/OE.28.002683

DO - 10.1364/OE.28.002683

M3 - Journal article

C2 - 32121951

VL - 28

SP - 2683

EP - 2698

JO - Optics Express

JF - Optics Express

SN - 1094-4087

IS - 3

ER -

ID: 247441611