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Conference on Design of Circuits and Integrated Systems

A 1.15 mW SiGe BiCMOS Cryogenic LNA for Superconducting Qubit Readout with 4.5 K Noise Temperature From 4 to 9 GHz

Aleksei Nerushenko, Roc Berenguer, Alvaro Urain, Héctor Solar

Published Nov 26, 2025• 1 citation
Publisher

Abstract

This work presents the design and post-layout simulation of a cryogenic SiGe BiCMOS low-noise amplifier (LNA) for superconducting transmon-qubit readout in quantum processors scaling beyond hundreds of qubits. The target specifications are first established and justified by surveying state-of-the-art of cryogenic LNAs and modeling the dispersive qubit readout process. The LNA is implemented with three cascaded stages in common-emitter configuration and employs tuned inductive matching and parallel peaking networks in each stage to optimize noise, gain flatness, and bandwidth while maintaining minimal DC power consumption. The amplifier draws only 1.15 mW from a 0.15 V supply and occupies$0.252 \text{mm}^{2}$. Post-layout simulations confirm input/output S-parameter matching better than$-10 \text{dB}, 41-44 \text{dB}$gain with$<3 \text{dB}$ripple,$<5 \mathrm{K}$noise temperature across$4-9 \text{GHz}$, and a worst-case OP1 dB compression point of$\mathbf{- 1 9. 9 6. 6 d B m}$. A comparative analysis demonstrates that SiGe BiCMOS offers a favorable trade-off between InP HEMT's low noise and CMOS's integration potential for large-scale quantum processors.

DOI
10.1109/dcis67520.2025.11281903

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A SiGe BiCMOS cryogenic direct-conversion receiver operating at 4 K is presented that demonstrates high-fidelity readout of a transmon qubit. Notably, at 6 mW, this design demonstrates a readout fidelity greater than 98% in1 μs\mathbf{1}\ \mu \mathbf{s}1 μswhen preceded by a Josephson parametric amplifier with a gain of 15–18 dB. To the best of the authors' knowledge, this is the first system that entirely replaces an InP-HEMT LNA-based receiver chain with a silicon readout integrated circuit. This demonstration represents an important step in the realization of fully integrated, large-scale cryogenic qubit control systems.
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