Abstract

High-fidelity single-shot readout of spin qubits requires distinguishing states much faster than the T1 time of the spin state. One approach to improving readout fidelity and bandwidth (BW) is cryogenic amplification, where the signal from the qubit is amplified before noise sources are introduced and room-temperature amplifiers can operate at lower gain and higher BW. We compare the performance of two cryogenic amplification circuits: a current-biased heterojunction bipolar transistor circuit (CB-HBT), and an AC-coupled HBT circuit (AC-HBT). Both circuits are mounted on the mixing-chamber stage of a dilution refrigerator and are connected to silicon metal oxide semiconductor (Si-MOS) quantum dot devices on a printed circuit board (PCB). The power dissipated by the CB-HBT ranges from 0.1 to 1 μW whereas the power of the AC-HBT ranges from 1 to 20 μW. Referred to the input, the noise spectral density is low for both circuits, in the 15 to 30 fA/sqrt{{bf{Hz}}} range. The charge sensitivity for the CB-HBT and AC-HBT is 330 μe/sqrt{{bf{Hz}}} and 400 μe/sqrt{{bf{Hz}}}, respectively. For the single-shot readout performed, less than 10 μs is required for both circuits to achieve bit error rates below 10−3, which is a putative threshold for quantum error correction.

Highlights

  • Spin qubits in semiconductors are a promising platform for building quantum computers[1,2,3,4,5,6,7,8]

  • The Coulomb blockade (CB)-heterojunction bipolar transistors (HBTs) has the drain of the single electron transistor (SET) connected to the base of the HBT, while the AC-coupled HBT circuit (AC-HBT) has the base of the HBT connected to the drain of the SET via a resistor-capacitor (RC) bias tee

  • The silicon metal oxide semiconductor (Si-MOS) device and HBT are mounted on a printed circuit board (PCB) only centimeters apart

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Summary

Introduction

Spin qubits in semiconductors are a promising platform for building quantum computers[1,2,3,4,5,6,7,8]. Te = 240 mK, gain = 2700 A/A, power = 13 μW, noise referred to input ≤70 fA/ Hz , and 350 μe/ Hz charge sensitivity[39]. The proximity of the HBT amplifier to the SET has the advantages of minimizing parasitic input capacitance and increasing signal before noise from the fridge is added.

Results
Conclusion

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