1.Sandia National Laboratories, Albuquerque, NM 87185, USA
2.Center for Integrated Nanotechnologies, Sandia National Laboratories, Albuquerque, NM 87185, USA
3.Max Planck Institute for the Science of Light, 91058 Erlangen, Germany
4.Friedrich-Alexander-Universität Erlangen-Nürnberg, 91058 Erlangen, Germany
Igal Brener (ibrener@sandia.gov)
收稿:2025-03-06,
修回:2025-07-11,
录用:2025-07-31,
网络出版:2025-10-17,
纸质出版:2025-12-31
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Jiho Noh, Tomás Santiago-Cruz, Chloe F. Doiron, 等. Fano interference of photon pairs from a metasurface[J]. Light: Science & Applications, 2025,14(12):3961-3968.
Noh, J. et al. Fano interference of photon pairs from a metasurface. Light: Science & Applications, 14, 3961-3968 (2025).
Jiho Noh, Tomás Santiago-Cruz, Chloe F. Doiron, 等. Fano interference of photon pairs from a metasurface[J]. Light: Science & Applications, 2025,14(12):3961-3968. DOI: 10.1038/s41377-025-01998-5.
Noh, J. et al. Fano interference of photon pairs from a metasurface. Light: Science & Applications, 14, 3961-3968 (2025). DOI: 10.1038/s41377-025-01998-5.
Two-photon interference
a quantum phenomenon arising from the principle of indistinguishability
is a powerful tool for quantum state engineering and plays a fundamental role in various quantum technologies. These technologies demand robust and efficient sources of quantum light
as well as scalable
integrable
and multifunctional platforms. In this regard
quantum optical metasurfaces
(QOMs) are emerging as promising platforms for the generation and engineering of quantum light
in particular pairs of entangled photons (biphotons) via spontaneous parametric down-conversion (SPDC). Due to the relaxation of the phase-matching condition
SPDC in QOMs allows different channels of biphoton generation
such as those supported by overlapping resonances
to occur simultaneously. In previously reported QOMs
however
SPDC was too weak to observe such effects. Here
we develop QOMs based on [110
]
-oriented GaAs that provide an order-of-magnitude enhancement in SPDC rate
after accounting for the spectral bandwidth
compared to any other QOMs studied to date. This boosted efficiency allows the QOMs to support the simultaneous generation of SPDC from several spectrally overlapping optical modes. Using a linear polarizer
we intentionally erase the distinguishability between the biphotons from a high-
Q
quasi-bound-state-in-the-continuum resonance and a low-
Q
Mie resonance
which results in the first-time observation of two-photon interference
shown in the form of a Fano contour
in the spectrum of biphotons. This quantum interference can enrich the generation of entangled photons in metasurfaces. Their advanced multifunctionality
improved nonlinear response
ease of fabrication
and compact footprint of [110
]
-GaAs QOMs position them as promising platforms to fulfill the requirements of photonic quantum technologies.
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