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Thin-film Diamond Photonic Crystal Cavities for the Tin-Vacancy Center

Hope Lee, Hannah Calzi Kleidermacher, Abigail Stein, Hyunseok Oh, Lillian Hughes Wyatt, Casey K. Kim, Mohamadali Malakoutian, Luca Basso, Andrew M. Mounce, Yongqiang Wang, Shei S. Shu, Michael Titze, Srabanti Chowdhury, Ania C. Bleszynski Jayich, Jelena Vuckovic A

Published Jan 1, 2026• 0 citations
Publisher

Abstract

We report the coupling of tin-vacancy centers (SnV − ) to 1D photonic crystal cavities in diamond thin-films; we observe a quality factor of ~ 6000 and a 10-fold PL enhancement.
DOI
10.1364/cleo_fs.2026.fm2c.5

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The negatively charged tin-vacancy center in diamond (SnV−^-−) is an excellent solid state qubit with optically-addressable transitions and a long electron spin coherence time at elevated (∼1.7\sim1.7∼1.7 K). However, implementing scalable quantum nodes with high-fidelity optical readout of the electron spin state requires efficient photon emission and collection from the system. In this manuscript, we report a quantum photonic interface for SnV−^-− centers based on one-dimensional photonic crystal cavities fabricated in diamond thin films. Furthermore, we provide a rigorous description of the spontaneous emission dynamics of our system, taking into account individual contributions from both the C and D transitions of the emitter. This allows for determination of Purcell factors per transition and, by extension, the C/D branching ratio SnV−^{-}− zero phonon line. We observe quality factors up to $\sim$6000 across this sample, and measure up to a 12-fold lifetime reduction, which translates into a Purcell factor of FC=26.2±1.5F_C=26.2\pm1.5FC​=26.2±1.5 for a targeted C transition. By considering the cavity mode polarization alignment with the C and D transition dipole moments, we validate the C/D branching ratio to be ηBR=0.75±0.01η_{\text{BR}}=0.75\pm0.01ηBR​=0.75±0.01, in line with previous theoretical and experimental findings.
We demonstrate optical coupling between a single tin-vacancy (SnV) center in diamond and a free-standing photonic crystal nanobeam cavity. The cavities are fabricated using quasi-isotropic etching and feature experimentally measured quality factors as high as ∼11 000. We investigate the dependence of a single SnV center's emission by controlling the cavity wavelength using a laser-induced gas desorption technique. Under resonance conditions, we observe an intensity enhancement of the SnV emission by a factor of 12 and a 16-fold reduction of the SnV lifetime. Based on the large enhancement of the SnV emission rate inside the cavity, we estimate the Purcell factor for the SnV zero-phonon line to be 37 and the coupling efficiency of the SnV center to the cavity, the β factor, to be 95%. Our work paves the way for the realization of quantum photonic devices and systems based on efficient photonic interfaces using the SnV color center in diamond.
The tin-vacancy center in diamond (SnV) has emerged as a compelling building block for realizing next-generation quantum networks thanks to its excellent optical and spin properties. Coupling to photonic crystal cavities (PCCs) promises to further enhance the SnV light-matter interface and unlock a diverse range of entanglement generation protocols. Recent pioneering experiments showing Purcell enhancement of SnV centers in PCCs underscore this potential. However, optical coupling that is coherent - the key ingredient for use in quantum protocols - has so far remained elusive. Here, we demonstrate above-unity coherent cooperativity of SnV centers embedded in photonic crystal cavities. We fabricate free-standing PCCs using a quasi-isotropic undercut. Across two samples, we conduct room-temperature characterizations, measuring resonances for 327 cavities, with an average quality factor exceeding Q=1.0(3)×104Q = 1.0(3) \times 10^4Q=1.0(3)×104. Two cavity-coupled emitters are examined in detail, exhibiting quality factors up to Q=25.4(4)×103Q = 25.4(4) \times 10^3Q=25.4(4)×103 and Purcell-reduced lifetimes corresponding to cooperativities up to C=20.6(11)C = 20.6(11)C=20.6(11). Furthermore, the single SnVs are observed to strongly modulate the cavity transmission with an extinction contrast up to 98.8(4)%98.8(4) \%98.8(4)% on resonance. Finally, SnV linewidth measurements reveal above-unity coherent cooperativities in both devices, with the highest value being Ccoh=8.3(12)C_\mathrm{coh} = 8.3(12)Ccoh​=8.3(12). These results open the door to using cavity-coupled SnV centers as efficient, coherent light-matter interfaces for future quantum networks.