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arXiv:2609.04150

Efficient Conversion of Optical to Mechanical States Close to the Single-Quantum Level

Alexander Rolf Korsch, Liu Chen, Pedro V. Pinho, Boris Müllendorff, Jan N. Kirchhof, Yong Yu, Thiago P. Mayer Alegre, Simon Gröblacher

quant-phSubmitted Sep 3, 2026• Announced Sep 4, 2026• 0 citations
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Abstract

Coherent interfaces between optical photons and mechanical excitations provide a promising route towards phonon-state engineering and hybrid quantum information processing. Cavity optomechanical systems enable such interfaces via optomechanically induced transparency (OMIT), allowing coherent mapping between traveling optical fields and localized mechanical modes. However, previous implementations of OMIT conversion protocols were limited to classical input signals with large coherent state photon numbers due to room temperature operation and corresponding thermal mechanical noise. Here, we demonstrate efficient low-noise photon-phonon state transfer close to the single-quantum regime in an optomechanical crystal operated at Millikelvin temperatures. Using weak coherent optical input pulses at the few-photon level, we achieve a record-level photon-phonon conversion efficiency of $η=0.76$, a mechanical storage lifetime of $T_\mathrm{1}=7.3~μs$, and a tunable conversion bandwidth exceeding 4.5 MHz. Hanbury Brown-Twiss measurements of the retrieved signal demonstrate the coherent nature of the converted phononic state, evidencing low added thermal noise in the conversion process ($n_\mathrm{th}=9.0$). These results establish optomechanical crystals as efficient optical interfaces to GHz mechanical modes and provide a pathway toward deterministic single-quantum-level mechanical state preparation.

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Coherent interfaces between optical photons and mechanical excitations provide a promising route towards phonon-state engineering and hybrid quantum information processing. Cavity optomechanical systems enable such interfaces via optomechanically induced transparency (OMIT), allowing coherent mapping between traveling optical fields and localized mechanical modes. However, previous implementations of OMIT conversion protocols were limited to classical input signals with large coherent state photon numbers due to room temperature operation and corresponding thermal mechanical noise. Here, we demonstrate efficient low-noise photon-phonon state transfer close to the single-quantum regime in an optomechanical crystal operated at Millikelvin temperatures. Using weak coherent optical input pulses at the few-photon level, we achieve a record-level photon-phonon conversion efficiency of η=0.76η=0.76η=0.76, a mechanical storage lifetime of T1=7.3 μsT_\mathrm{1}=7.3~μsT1​=7.3 μs, and a tunable conversion bandwidth exceeding 4.5 MHz. Hanbury Brown-Twiss measurements of the retrieved signal demonstrate the coherent nature of the converted phononic state, evidencing low added thermal noise in the conversion process (nth=9.0n_\mathrm{th}=9.0nth​=9.0). These results establish optomechanical crystals as efficient optical interfaces to GHz mechanical modes and provide a pathway toward deterministic single-quantum-level mechanical state preparation.
Optomechanical crystals (OMCs) enable coherent interactions between optical photons and microwave acoustic phonons, and represent a platform for implementing quantum transduction between microwave and optical signals. Optical-absorption-induced thermal noise at cryogenic (millikelvin) temperatures is one of the primary limitations of performance for OMC-based quantum transducers. Here, we address this challenge with a two-dimensional silicon OMC resonator that is side-coupled to a mechanically detached optical waveguide, realizing a six-fold reduction in the heating rate of the acoustic resonator compared to prior state-of-the-art, while operating in a regime of high optomechanical-backaction and millikelvin base temperature. This reduced heating translates into a demonstrated phonon-to-photon conversion efficiency of 93.1±0.8% at an added noise of 0.25±0.01 quanta, representing a significant advance toward quantum-limited microwave-optical frequency conversion and optically controlled quantum acoustic memories.
Abstract Nano-structured optomechanical crystals (OMC) form an interface between mechanical modes with long coherence times and telecom optical photons, ideal for long-distance distribution of quantum information. However, the implementation of scalable quantum networks based on OMCs has been inhibited by thermal mechanical noise. Here, we overcome this limitation using a quasi-two-dimensional OMC and generate single photons via single phonon-photon conversion. In this work, we verify the low thermal noise and high purity of the generated single photons through a Hanbury Brown-Twiss experiment with g(2)(0)=0.35−0.08+0.10{g}^{(2)}(0)=0.3{5}_{-0.08}^{+0.10}g(2)(0)=0.35−0.08+0.10​ g ( 2 ) ( 0 ) = 0.3 5 − 0.08 + 0.10 . We perform Hong-Ou-Mandel interference of the emitted photons showcasing the indistinguishability and coherence with visibility V = 0.52 ± 0.15 after 1.43 km fiber delay. Lastly, we use two-photon interference to measure the temporal wavepackets of optomechanically generated single photons demonstrating narrow bandwidths as low as 10 MHz. Our results pave the way for multinode quantum networks of mechanical oscillators and hybrid entanglement generation between mechanical oscillators and telecom quantum emitters.
We demonstrate a memory for light based on optomechanically induced transparency. We achieve a long storage time by leveraging the ultra-low dissipation of a soft-clamped mechanical membrane resonator, which oscillates at MHz frequencies. At room temperature, we demonstrate a lifetime T1≈23 msT_1 \approx 23\,\mathrm{ms}T1​≈23ms and a retrieval efficiency η≈40%η\approx 40\%η≈40% for classical coherent pulses. We anticipate storage of quantum light to be possible at moderate cryogenic conditions (T≈10 KT\approx 10\,\mathrm{K}T≈10K). Such systems could find applications in emerging quantum networks, where they can serve as long-lived optical quantum memories by storing optical information in a phononic mode.
Noise is an ever-present reality of the world we live in. From the non-deterministic movement of matter to the fluctuations of the physical fields surrounding us, noise is the ultimate adversary of all things pure. Noise limits the fidelity of information transfer, particularly for quantum signals relying on coherence. Yet at sufficiently low temperatures, ambient thermal noise is suppressed to a level where even quantum signals can maintain coherence, making them available for technological applications. Modern cryogenic technologies enable access to environmental temperatures of 10 mK, allowing quantum-coherent transfer and processing of signals with carrier frequencies in the GHz range.A technology that operates in this regime is the optomechanical crystal: a nanofabricated device that supports high-quality resonances for both optical and acoustic fields and enables coherent coupling between the two. Through the optomechanical interaction, the acoustic mode can serve as a universal bus for the optical field, coherently linking it to other nonlinear systems, such as superconducting qubits – thereby enabling quantum microwave-to-optical transduction. As with many quantum systems, however, device performance is constrained by excess noise. In optomechanical crystals, this noise primarily stems from optical absorption combined with insufficient thermal anchoring. Achieving robust quantum-level operation in future devices therefore requires a detailed understanding and careful mitigation of these noise mechanisms.This thesis makes progress toward overcoming optical-absorption-induced noise in optomechanical crystals by (I) introducing a new class of optomechanical devices with superior thermal anchoring: the release-free optomechanical crystal; and (II) carefully investigating its noise performance and potential for microwave-to-optical transduction. The results presented in this thesis contribute to the understanding of noise limits in silicon optomechanical crystals and showcase the release-free platform as a viable alternative for on-chip, low-noise optomechanics.
We demonstrate a memory for light based on optomechanically induced transparency. We achieve a long storage time by leveraging the ultralow dissipation of a soft-clamped mechanical membrane resonator, which oscillates at MHz frequencies. At room temperature, we demonstrate a lifetime ${T}_{1}\ensuremath{\approx}23\text{ }\text{ }\mathrm{ms}$ and a retrieval efficiency $\ensuremath{\eta}\ensuremath{\approx}40%$ for classical coherent pulses. We anticipate the storage of quantum light to be possible at moderate cryogenic conditions ($T\ensuremath{\approx}10\text{ }\text{ }\mathrm{K}$). Such systems could find applications in emerging quantum networks, where they can serve as long-lived optical quantum memories by storing optical information in a phononic mode.
Scalable quantum networks require quantum memories that are chip-integrated, telecom-band compatible, and capable of flexible retrieval. Nanofabricated mechanical resonators meet these criteria. They offer independent tunability of optical and mechanical modes, long-lived phonon states, and design flexibility beyond atomic systems, making them strong candidates for practical integrated quantum memory. Here, we demonstrate an on-chip, absorptive optomechanical memory for telecom-band photons, based on optomechanically induced transparency (OMIT) and operating near the mechanical ground state. The device stores telecom-band photons, demonstrating compatibility with external photon sources at the few-photon level, while enabling on-demand retrieval. By placing the device in a dilution refrigerator at 20 mK and tailoring the control field to suppress optical heating, we achieve a remarkably low phonon occupancy of just 0.32 during the storage process. Our results lay the groundwork for scalable, phonon-based quantum memory devices and open new avenues for integrating mechanical systems into practical quantum network architectures.