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arXiv:2608.29435

Parametric amplification in a Kerr Oscillator based on Ne FIB Nanobridges

Parth Bhandari, Laith Meti, Gemma Chapman, Edward Romans, John Gallop, Ling Hao

quant-phcond-mat.supr-conSubmitted Aug 29, 2026• Announced Sep 1, 2026• 0 citations
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Abstract

Superconducting circuits play a crucial role in the advancement of quantum computing and quantum sensing. Typically such circuits require the presence of a non-linear element, where the engineered anharmonicity (Kerr factor) and resonant linewidth determine the potential applications of the circuit. In this work we have fabricated Nb-based CPW resonators embedded with a DC SQUID incorporating Nb nanobridges as the weak links. We use two-tone spectroscopy to study the non-linear behaviour of the device at 15 mK up to a field of 2.48 mT. Under the application of a blue-detuned pump, the device shows a decrease in the resonant frequency which is used to estimate the Kerr factor. We further apply a red-detuned pump to go beyond the bifurcation threshold and observe the appearance of an additional idler mode with net gain. The gain of the device was maximized by further decreasing the pump frequency, showing a maximum amplification of 15 dB. Finally, we show agreement between the Kerr non-linear oscillator model and the measured transmission spectrum, and highlight further design modifications to improve the gain and bandwidth of such devices.

AI Summary

The paper investigates four-wave-mixing parametric amplification in a Nb nanobridge SQUID resonator, motivated by alternatives to Al devices for magnetic-field-exposed microwave applications. The device is a $\lambda/4$ CPW resonator terminated by a DC SQUID whose weak links are patterned using Ne focused-ion-beam lithography. Measurements at $15\,\mathrm{mK}$ characterize a resonance near $5.627\,\mathrm{GHz}$, with low-power internal and external quality factors of $7.4\times10^4$ and $4.5\times10^4$. Blue-detuned pump–probe spectroscopy measures the pump-induced resonance shift. Iterative fitting to the steady-state photon-number equation and linearized signal–idler response of a Kerr oscillator gives a zero-field Kerr factor of $-2.14\,\mathrm{mHz/photon}$, close to a circuit estimate of $-2.13\,\mathrm{mHz/photon}$. The Kerr response persists in perpendicular fields up to $2.48\,\mathrm{mT}$. Red-detuned pumping produces a signal–idler response, with separate spectrum-analyzer measurements verifying $\omega_s+\omega_i=2\omega_p$. Sweeping the pump frequency along the high-photon-number branch yields a maximum transmission gain of $15\,\mathrm{dB}$ relative to the measured baseline, with approximately $300\,\mathrm{kHz}$ bandwidth. A standard driven-Kerr input–output model reproduces the principal spectral features and branch switching. The field-dependent measurements establish nonlinear response rather than amplifier performance at the maximum field. Above $2.48\,\mathrm{mT}$, pump-dependent frequency jumps are attributed to vortex motion. Added noise and dynamic range remain unmeasured; stronger overcoupling and lower resonator quality factor are proposed to improve gain and bandwidth.

Little sign of AI-generated textIncremental

Error found: The initial intracavity photon-number estimate is too large by a factor of 2π relative to the paper's own cubic equation in the zero-detuning, negligible-Kerr limit, although its use only as an initial guess limits the consequence.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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Superconducting circuits play a crucial role in the advancement of quantum computing and quantum sensing. Typically such circuits require the presence of a non-linear element, where the engineered anharmonicity (Kerr factor) and resonant linewidth determine the potential applications of the circuit. In this work we have fabricated Nb-based CPW resonators embedded with a DC SQUID incorporating Nb nanobridges as the weak links. We use two-tone spectroscopy to study the non-linear behaviour of the device at 15 mK up to a field of 2.48 mT. Under the application of a blue-detuned pump, the device shows a decrease in the resonant frequency which is used to estimate the Kerr factor. We further apply a red-detuned pump to go beyond the bifurcation threshold and observe the appearance of an additional idler mode with net gain. The gain of the device was maximized by further decreasing the pump frequency, showing a maximum amplification of 15 dB. Finally, we show agreement between the Kerr non-linear oscillator model and the measured transmission spectrum, and highlight further design modifications to improve the gain and bandwidth of such devices.
The paper investigates four-wave-mixing parametric amplification in a Nb nanobridge SQUID resonator, motivated by alternatives to Al devices for magnetic-field-exposed microwave applications. The device is a λ/4\lambda/4λ/4 CPW resonator terminated by a DC SQUID whose weak links are patterned using Ne focused-ion-beam lithography. Measurements at 15 mK15\,\mathrm{mK}15mK characterize a resonance near 5.627 GHz5.627\,\mathrm{GHz}5.627GHz, with low-power internal and external quality factors of 7.4×1047.4\times10^47.4×104 and 4.5×1044.5\times10^44.5×104.
Blue-detuned pump–probe spectroscopy measures the pump-induced resonance shift. Iterative fitting to the steady-state photon-number equation and linearized signal–idler response of a Kerr oscillator gives a zero-field Kerr factor of −2.14 mHz/photon-2.14\,\mathrm{mHz/photon}−2.14mHz/photon, close to a circuit estimate of −2.13 mHz/photon-2.13\,\mathrm{mHz/photon}−2.13mHz/photon. The Kerr response persists in perpendicular fields up to 2.48 mT2.48\,\mathrm{mT}2.48mT. Red-detuned pumping produces a signal–idler response, with separate spectrum-analyzer measurements verifying ωs+ωi=2ωp\omega_s+\omega_i=2\omega_pωs​+ωi​=2ωp​. Sweeping the pump frequency along the high-photon-number branch yields a maximum transmission gain of 15 dB15\,\mathrm{dB}15dB relative to the measured baseline, with approximately 300 kHz300\,\mathrm{kHz}300kHz bandwidth. A standard driven-Kerr input–output model reproduces the principal spectral features and branch switching.
The field-dependent measurements establish nonlinear response rather than amplifier performance at the maximum field. Above 2.48 mT2.48\,\mathrm{mT}2.48mT, pump-dependent frequency jumps are attributed to vortex motion. Added noise and dynamic range remain unmeasured; stronger overcoupling and lower resonator quality factor are proposed to improve gain and bandwidth.
Recently the exploration of nonlinear microwave response in superconducting circuits has been extended to Nb nanobridges that can operate at higher magnetic fields, frequencies, and temperatures than their conventional Al counterparts. Nb nanobridge-based Superconducting Quantum Interference Devices (SQUIDs) have shown potential applications in quantum information processing, weak signal detection, and single spin detection. Combining such non-linear elements with circuit Quantum Electrodynamic (QED) elements like coplanar waveguide (CPW) resonators allows the study of the nonlinearity of such systems. In this work we report on the design, fabrication and dispersive microwave readout of a Nb DC nanoSQUID embedded in a superconducting quarter-wavelength resonator. The measured flux-tuneability of the resonance shows a modulation of a few MHz and fits simulations, giving a critical current of 330 μA and a screening parameterβLof 4.07. Following this we present results showing Kerr-type detuning with a pump tone applied to the device.
In this licentiate thesis, I present the design, fabrication, and characterization of superconducting parametric resonators, for use in quantum information processing. These devices are quarter-wavelength coplanar waveguide resonators (~5 GHz), terminated at one end by a non-linear inductance provided by a SQUID (superconducting quantum interference device). The SQUID acts as a flux-controlled boundary condition, which effectively changes the electrical length of the resonator. This enables the modulation of the resonant frequency by coupling microwave magnetic flux into the SQUID, using on-chip transmission lines. The modulation occurs on a timescale much faster than the photon loss out of the resonator. The non-linearity provides several different regimes for operating this device. I focused on the parametric regime, in which the non-linear element was being modulated (pumped) at or near twice the resonant frequency. This pumping can lead to amplification and frequency conversion of an incoming signal. It can also give rise to instabilities and self-oscillations "parametric oscillations" - that is, the generation of an intense electric field in the resonator (the creation of photons). Parametric oscillations set in when the pumping strength exceeds a threshold value, and also depends on the pump-frequency detuning from twice the resonance and on the static flux through the SQUID. I characterized the devices over a wide parameter range by doing homodyne detection of the reflected signal or of the emitted field oscillations. In particular, I investigated the damping and two leading nonlinearities, dominating in different operating regimes, which influence the dynamics of the parametric resonator. First, I extracted the Duffing nonlinearity by studying the line width of the resonator as a function of the input signal (without pumping the SQUID). Second, with high pump amplitude, I extracted the pump-induced nonlinearity by determining the threshold parameters (pump amplitude and detuning) for the onset of parametric oscillations; this nonlinearity leads to the generation of higher-order pump terms that complicate the system dynamics, but can be mitigated now that they have been understood. My results validate a recent theoretical model for the classical, non-linear dynamics of parametric resonance, and helps determine workable design parameters. Finally, I helped develop a linearized model −-− the "pumpistor" - describing this device in terms of a flux-controlled impedance. This will be useful when designing more complex circuits. One goal of this work is to demonstrate single-shot measurements on superconducting qubits (quantum bits of information). We will use the parametric resonator as a threshold discriminator, associating the qubit's two energy eigenstates with the parametric oscillations either turning on or not. This would be a very useful device in the quantum engineer's toolbox when designing systems for quantum information processing and communication.
Parametric amplification is essential for quantum measurement, enabling the amplification of weak microwave signals with minimal added noise. While Josephson-junction-based amplifiers have become standard in superconducting quantum circuits, their magnetic sensitivity, limited saturation power, and sub-kelvin operating requirements motivate the development of alternative nonlinear platforms. Here we demonstrate a two-mode kinetic-inductance parametric amplifier based on a pair of capacitively coupled Kerr-nonlinear resonators fabricated from NbTiN and NbN thin films. The distributed Kerr nonlinearity of these materials enables nondegenerate four-wave-mixing amplification with gains approaching 40 dB, gain-bandwidth products up to 6.9 MHz, and 1-dB compression powers two to three orders of magnitude higher than those of state-of-the-art Josephson amplifiers. A coupled-mode theoretical model accurately captures the pump-induced modification of the hybridized modes and quantitatively reproduces the observed signal and idler responses. The NbN device exhibits a significantly larger Kerr coefficient and superior gain-bandwidth performance, highlighting the advantages of high-kinetic-inductance materials. Our results establish coupled kinetic-inductance resonators as a robust platform for broadband, high-power, and magnetically resilient quantum-limited amplification, offering a scalable route for advanced readout in superconducting qubits, spin ensembles, quantum dots, and other microwave-quantum technologies.
Abstract Superconducting resonator parametric amplifiers are potentially important components for a wide variety of fundamental physics experiments and utilitarian applications. We propose and realise an operating scheme that achieves amplification through the use of non-degenerate pumps, which addresses two key challenges in the design of parametric amplifiers: non-continuous gain across the amplification band and pump tone removal. We have experimentally demonstrated the non-degenerate pumping scheme using a half-wave resonator amplifier based on NbN thin-film, and measured a peak gain of 26 dB and 3-dB bandwidth of 0.5 MHz. The two non-degenerate pump tones were positioned ∼10\sim 10∼10 ∼ 10 bandwidths above and below the frequency at which peak gain occurs. We have found the non-degenerate pumping scheme to be more stable compared to the usual degenerate pumping scheme in terms of gain drift over time, by a factor of 4. This scheme also retains the usual flexibility of NbN resonator parametric amplifiers in terms of reliable amplification in a ∼4\sim 4∼4 ∼ 4 K environment, and is suitable for cross-harmonic amplification. The use of pump tones at different frequencies allows phase-sensitive amplification when the signal tone is degenerate with the idler tone. A gain of 23 dB and squeezing ratio of 6 dB were measured.
Nonlinear microwave resonators are a versatile tool in quantum information processing, enabling parametric amplification, continuous variable quantum computing, and engineered mode interactions. Many of these applications especially benefit from cubic nonlinearities enabling three-wave mixing; at the same time, they are limited by quartic nonlinearities giving rise to undesired Kerr effects. A recurrent challenge is therefore to engineer resonators with a finite cubic nonlinearity while suppressing quartic terms. Here, we investigate a superconducting resonator hosting two weak links fabricated from an aluminum-capped indium arsenide nanowire. We characterize the Kerr nonlinearity as a function of magnetic flux and gate bias, showing that it can be tuned to zero with either control parameter. Furthermore, we experimentally demonstrate three-wave mixing in a semiconductor-superconductor hybrid device, establishing nonzero cubic nonlinearity. An effective model based on Andreev bound states qualitatively captures the observed trends. Our results validate semiconductor-superconductor hybrid devices as a promising platform for tunable nonlinear superconducting circuits, with applications in parametric amplification, quantum control of bosonic modes, and engineering interactions between microwave modes.
Abstract Modern parametric amplifiers are based on lithographically produced superconducting thin-film planar transmission line structures. These paramps rely on resonant structures with embedded nonlinear elements to stimulate intermodulation with a stronger pump tone that gives rise to signal gain when certain conditions are satisfied. Such paramps have not yet been realised in superconducting 3D waveguide resonators. Possible applications of these devices include detector systems that are based on 3D waveguide such as dark matter detectors and quantum computers. Reported here are the results of an investigation of a 30.64 GHz series circular waveguide resonance machined from bulk niobium showing parametric gain of up to 2 dB in the presence of a stronger pump tone 10 kHz above in frequency. The gain is largest on abrupt jumps of the transmission spectra of the resonance, which may be a result of weak-link formation on the superconducting surfaces.