Expanding to higher qubit frequencies introduces the challenge of routing >20 GHz signals into a dilution refrigerator without adding excess thermal load or frequency-dependent loss. In this work, we demonstrate a solution to this problem by using a frequency multiplier to drive the qubit with room-temperature control pulses at half or one third of the qubit frequency fQB. The control pulses are up-converted inside the cryogenic environment using a frequency multiplier based on a high-kinetic inductance nonlinear transmission line. We evaluated the success of the upconversion technique by comparing the randomized benchmarking error-per-gate metrics to that of a standard direct qubit driving technique. The fQB=2 drive technique achieved error rates consistent with the direct drive, with a minimum error per gate of 3:5 � 10−3 6 0:4 � 10−3. The fQB=3 drive technique resulted in a minimum error per gate of 7:6 � 10−3 6 0:81 � 10−3. While this demonstration is based around a fQB ¼ 4:836 GHz qubit so that a direct drive comparison is possible, this technique will allow higherfrequency qubits to be tested using existing radio frequency infrastructure.
Giesbrecht, G., Castellanos-Beltran, M., Sirois, A., Flowers-Jacobs, N., Olaya, D., Vissers, M., et al. (2026). Superconducting qubit control using cryogenic frequency conversion. APPLIED PHYSICS LETTERS, 129(3) [10.1063/5.0335299].
Superconducting qubit control using cryogenic frequency conversion
Giachero, A.;
2026
Abstract
Expanding to higher qubit frequencies introduces the challenge of routing >20 GHz signals into a dilution refrigerator without adding excess thermal load or frequency-dependent loss. In this work, we demonstrate a solution to this problem by using a frequency multiplier to drive the qubit with room-temperature control pulses at half or one third of the qubit frequency fQB. The control pulses are up-converted inside the cryogenic environment using a frequency multiplier based on a high-kinetic inductance nonlinear transmission line. We evaluated the success of the upconversion technique by comparing the randomized benchmarking error-per-gate metrics to that of a standard direct qubit driving technique. The fQB=2 drive technique achieved error rates consistent with the direct drive, with a minimum error per gate of 3:5 � 10−3 6 0:4 � 10−3. The fQB=3 drive technique resulted in a minimum error per gate of 7:6 � 10−3 6 0:81 � 10−3. While this demonstration is based around a fQB ¼ 4:836 GHz qubit so that a direct drive comparison is possible, this technique will allow higherfrequency qubits to be tested using existing radio frequency infrastructure.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.


