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Bolometer operating at the threshold for circuit quantum electrodynamics

Abstract

Radiation sensors based on the heating effect of absorbed radiation are typically simple to operate and flexible in terms of input frequency, so they are widely used in gas detection1, security2, terahertz imaging3, astrophysical observations4 and medical applications5. Several important applications are currently emerging from quantum technology and especially from electrical circuits that behave quantum mechanically, that is, circuit quantum electrodynamics6. This field has given rise to single-photon microwave detectors7,8,9 and a quantum computer that is superior to classical supercomputers for certain tasks10. Thermal sensors hold potential for enhancing such devices because they do not add quantum noise and they are smaller, simpler and consume about six orders of magnitude less power than the frequently used travelling-wave parametric amplifiers11. However, despite great progress in the speed12 and noise levels13 of thermal sensors, no bolometer has previously met the threshold for circuit quantum electrodynamics, which lies at a time constant of a few hundred nanoseconds and a simultaneous energy resolution of the order of 10h gigahertz (where h is the Planck constant). Here we experimentally demonstrate a bolometer that operates at this threshold, with a noise-equivalent power of 30 zeptowatts per square-root hertz, comparable to the lowest value reported so far13, at a thermal time constant two orders of magnitude shorter, at 500 nanoseconds. Both of these values are measured directly on the same device, giving an accurate estimation of 30h gigahertz for the calorimetric energy resolution. These improvements stem from the use of a graphene monolayer with extremely low specific heat14 as the active material. The minimum observed time constant of 200 nanoseconds is well below the dephasing times of roughly 100 microseconds reported for superconducting qubits15 and matches the timescales of currently used readout schemes16,17, thus enabling circuit quantum electrodynamics applications for bolometers.

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Fig. 1: Bolometer and its operation principle.
Fig. 2: Sample characterization data.
Fig. 3: Key performance indicators of the bolometer.

Data availability

Data supporting the findings of this study are available at https://zenodo.org/record/3978419.

Code availability

The algorithms used for the findings of this study are available within the paper and its Supplementary Information files.

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Acknowledgements

We acknowledge the provision of facilities and technical support by Aalto University at OtaNano – Micronova Nanofabrication Center and LTL Infrastructure, which is part of the European Microkelvin Platform (EMP, number 824109 EU Horizon 2020). We have received funding from the European Research Council under Consolidator Grant number 681311 (QUESS) and under Advanced Grant number 670743 (QuDeT), the European Commission through the H2020 programme project QMiCS (grant agreement 820505, Quantum Flagship), the Academy of Finland through its Centres of Excellence Programme (project numbers 312300, 312059 and 312295) and grants (numbers 314447, 314448, 314449, 305237, 316551, 308161, 335460, and 314302), the Finnish Cultural Foundation and the Vilho, Yrjö and Kalle Väisälä Foundation of the Finnish Academy of Science and Letters. We thank W. Liu and L. Grönberg for assistance in nanofabrication and for useful discussions.

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Contributions

R.K. and J.-P.G. conducted the experiments and data analysis of the data presented in the main article. The main sample was designed by R.E.L. and fabricated by D.H. and A.L. Initial characterizations were carried out by I.S., D.H. and J.G. Most of the measurement code was written by V.V. and J.G. Furthermore, J.Y.T. and K.W.C. fabricated the sample discussed in Supplementary Note I, which was measured and analysed by M.P. and K.Y.T. The sample presented in Supplementary Note II was produced by R.E.L. and A.L., and measured mainly by J.G. The manuscript was written by R.K., J.-P.G. and M.M. with comments from all authors. The work was supervised by P.H. and M.M.

Corresponding author

Correspondence to M. Möttönen.

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Extended data figures and tables

Extended Data Fig. 1 Controlled shift of the resonance frequency.

a, Measured reflection amplitude of the bolometer as a function of the probe frequency and the gate voltage at Pp = 17.4 aW. b, Reflection amplitude as a function of the probe frequency and power at Vg = 0 V. In each panel and each horizontal trace, the point of the lowest reflection amplitude roughly yields the resonance frequency. The bath temperature is Tb = 55 mK and no heater power is applied.

Extended Data Fig. 2 Responsivity and average noise density.

ac, Quasistatic responsivity (black markers, left axis) and noise density averaged over the frequency range 102–104 Hz (red markers, right axis) as functions of the probe frequency for gate voltages –2.5 V (a), 0 V (b) and 2.5 V (c). Dividing the noise density with the responsivity yields the NEP shown in Fig. 3. The bath temperature is Tb = 55 mK.

Extended Data Fig. 3 On-chip details of the bolometer.

Optical image of the bolometer, indicating the locations of capacitors C1, C2 and Cg. The transmission line at the centre left and the absorber gate line at the top left were not used in the experiment. The scale bar denotes 100 μm.

Extended Data Fig. 4 Detailed measurement setup.

The blue rectangle corresponds to the SEM image displayed in Fig. 1a. The model numbers on the filters, couplers and amplifiers refer to Mini-Circuits product numbers. Nominal temperatures of the different cryostat plates (dashed horizontal lines) are indicated. The 180° bends and spirals refer to long segments in the coaxial microwave cables and Thermocoax cables, respectively, which function as thermal bottlenecks separating the different temperature stages. The top-most dashed line refers to the boundary of the cryostat. The nested millikelvin radiation shields are made of gold-plated copper.

Extended Data Fig. 5 Calibration of the heater power.

Gain (left axis) and noise temperature (right axis) of the amplification chain from the microwave switch shown in Extended Data Fig. 4 to the room-temperature mixer, transmission amplitude from the heater signal generator to the mixer (left axis), and attenuation of the heater line from the signal generator to the switch (left axis) as functions of heater frequency. The error bars denote 1σ confidence intervals.

Extended Data Fig. 6 Response to heater power.

a–c, Difference in the voltage of the measured probe signal quadrature between heater-on and heater-off conditions as a function of the heater power level in the on state for gate voltage –2.5 V (a), 0 V (b) and 2.5 V (c) at the probe power and frequency for which we find the lowest NEP in Fig. 3. The solid line shows a linear fit up to a heating power of 16 aW (a) and 4 aW (b, c). The error bars denote 1σ confidence intervals.

Extended Data Fig. 7 Schematic cross sections of the bolometer.

a, Optical image of the bolometer. Grey colour indicates unused structures in our experiment. The boundary of the graphene flake is denoted by the dotted quadrangle. The scale bar denotes 5 μm. b, Schematic cross-sections of the bolometer along the dashed lines of the optical image (not to scale).

Extended Data Table 1 Parameters of the polynomial fitting function Pappl = [p1(Tb/K)3 + p2(Tb/K)2 + p3Tb/K + p4] fW for Fig. 2a

Supplementary information

Supplementary Information

This Supplementary Information file contains the following sections: Supplementary Methods I: Circuit model; Supplementary Note I: Switching of a proximity Josephson junction; Supplementary Note II: Mode shift of an SGS junction; and Supplementary References.

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Kokkoniemi, R., Girard, JP., Hazra, D. et al. Bolometer operating at the threshold for circuit quantum electrodynamics. Nature 586, 47–51 (2020). https://doi.org/10.1038/s41586-020-2753-3

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