Devices that achieve nonreciprocal microwave transmission are ubiquitous in radar and radio-frequency communication systems, and commonly rely on magnetically biased ferrite materials.Such devices are also indispensable in the readout chains of superconducting quantum circuits as they protect sensitive quantum systems from the noise emitted by readout electronics. Since ferrite-based nonreciprocal devices are bulky, lossy, and re- quire large magnetic fields, there has been significant interest in magnetic-field-free on-chip alternatives, such as those recently implemented using Josephson junctions. Here we realize reconfigurable nonreciprocal transmission between two microwave modes using purely optomechanical interactions in a superconducting electromechanical circuit. The scheme relies on purposely breaking the symmetry between two mechanically-mediated dissipative coupling pathways. This enables reconfigurable nonreciprocal isolation on-chip without any external magnetic field, rendering it fully compatible with superconducting quantum circuits. All-optomechanically- mediated nonreciprocity demonstrated here can be extended to implement other types of devices such as directional amplifiers and circulators, and it forms the basis towards realizing topological states of light and sound.
Dissipation can significantly affect the quantum behaviour of a system and even completely suppress it. Counterintuitively, engineered dissipation enables the preparation of quantumstates as well as their stabilization. In cavity electro- and optomechanics, the control over mechanical oscillators relies on a dissipation hierarchy in which the electromagnetic energy decay rate significantly exceeds that of the mechanical oscillator. In contrast, recent theoretical work has considered the opposite regime in which the mechanical oscillator dissipation dominates and provides a cold dissipative reservoir to the electromagnetic degree of freedom. This novel regime allows to manipulate the electromagnetic mode and enables a new class of dissipative interactions. Here, we report on the experimental realization of this reversed dissipation regime in a microwave cavity optomechanical system. We directly evidence the preparation of a quasi-instantaneous, cold reservoir for a microwave field by on-demand decreasing or increasing the damping rate of the microwave mode, that corresponds to amplification and de-amplification of the microwave field. Moreover, we observe the onset of parametric instability, i.e. stimulated emission of microwaves (masing). The dissipative interaction additionally enables to operate the system as a low-noise, large-gain phase-preserving amplifier. Realizing a dissipative reservoir for microwave light is a requirement for the dissipative coupling of multiple cavity modes, which in turn forms the basis of dissipative quantum phase transitions, microwave entanglement schemes, and electromechanical quantum-limited amplifiers. Equally importantly, this interaction underpins recently predicted non-reciprocal devices, which would extend the available toolbox of quantum-limited microwave manipulation techniques.