Abstract
Mechanical systems are pivotal in quantum technologies because of their long coherent time and versatile coupling to qubit systems. So far, the coherent and dynamic control of gigahertz-frequency mechanical modes mostly relies on optomechanical coupling and piezoelectric coupling to superconducting qubits. Here, we demonstrate on-chip cavity electroacoustic dynamics using our microwave-frequency electrically modulated phononic crystal resonators on lithium niobate. Leveraging the high dispersion of phononic crystal, our acoustic modes space unevenly in the frequency spectrum, emulating atomic energy levels. Atomiclike transitions between different acoustic modes are selectively achieved by applying electrical fields to modulate acoustic modes via the nonlinear piezoelectricity of lithium niobate. Among two modes, we demonstrate Autler-Townes splitting, ac Stark shift, and Rabi oscillation with a maximum cooperativity of 4.18. Extending to three modes, we achieve nonreciprocal frequency conversions with an isolation up to 20 dB. Nonreciprocity can be tuned by the time delay between the two modulating pulses. Our cavity electroacoustic platform could find broad applications in sensing, microwave signal processing, acoustic computing, and quantum acoustics.
| Original language | English |
|---|---|
| Article number | 227001 |
| Journal | Physical Review Letters |
| Volume | 136 |
| Issue number | 22 |
| DOIs | |
| State | Published - Jun 5 2026 |
Funding
We thank Rohde & Schwarz for support with microwave instrumentation. Device fabrication was conducted at the Center for Nanophase Materials Sciences (CNMS2022-B-01473, CNMS2024-B-02643, L. S.), which is a U.S. Department of Energy Office of Science User Facility. Research was partially supported by the Air Force Office of Scientific Research (AFOSR) under Grant No. W911NF-23-1-0235 (L. S.). Development of the optical vibrometer was partially supported by the Defense Advanced Research Projects Agency (DARPA) OPTIM program under Contract No. HR00112320031 (L. S. and Y. Z.). Design and simulation of the acoustic device were partially supported by DARPA SynQuaNon DO program under Agreement HR00112490314 (L. S.). We thank Rohde & Schwarz for support with microwave instrumentation. Device fabrication was conducted at the Center for Nanophase Materials Sciences (CNMS2022-B-01473, CNMS2024-B-02643, L. S.), which is a U.S. Department of Energy Office of Science User Facility. Research was partially supported by the Air Force Office of Scientific Research (AFOSR) under Grant No. W911NF-23-1-0235 (L. S.). Development of the optical vibrometer was partially supported by the Defense Advanced Research Projects Agency (DARPA) OPTIM program under Contract No. HR00112320031 (L. S. and Y. Z.). Design and simulation of the acoustic device were partially supported by DARPA SynQuaNon DO program under Agreement HR00112490314 (L. S.).
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