TY - JOUR
T1 - Interfacing Superconducting Qubits with Cryogenic Logic
T2 - Readout
AU - Howington, Caleb
AU - Opremcak, Alex
AU - McDermott, Robert
AU - Kirichenko, Alex
AU - Mukhanov, Oleg A.
AU - Plourde, Britton L.T.
N1 - Funding Information:
National Science Foundation under Grants QIS-1720304 and QIS-1720312
Funding Information:
Manuscript received October 30, 2018; accepted March 10, 2019. Date of publication April 2, 2019; date of current version May 17, 2019. This work was supported by the U.S. Government under Grant W911NF-15-1-0248. The work of R. McDermott and B. L. T. Plourde was supported by the National Science Foundation under Grants QIS-1720304 and QIS-1720312, respectively. (Corresponding author: Caleb Howington.) C. Howington and B. L. T. Plourde are with the Department of Physics, Syracuse University, Syracuse, NY 13244 USA (e-mail:, cjhowing@syr.edu; bplourde@syr.edu).
Publisher Copyright:
© 2002-2011 IEEE.
PY - 2019/8
Y1 - 2019/8
N2 - As superconducting quantum processors increase in size and complexity, the scalability of standard techniques for qubit control and readout becomes a limiting factor. Replacing room temperature analog components with cryogenic digital components could allow for the realization of systems well beyond the current state-of-The-Art qubit arrays with tens of qubits. The standard technique for performing a qubit measurement with heterodyne readout uses a quantum-limited cryogenic amplifier chain and requires bulky microwave components inside the refrigerator with multiple control lines and pump signals. Additionally, the result is only accessible in software at room temperature. An alternative method for measuring qubits involves mapping the qubit state onto the photon occupation in a microwave cavity, followed by subsequent photon detection using a Josephson photomultiplier (JPM). The JPM measures the qubit and stores the result in a classical circulating current. To make use of this result, we can leverage existing single flux quantum (SFQ) circuitry. An underdamped Josephson transmission line (JTL) can be coupled to the JPM and fluxons traveling along the JTL are accelerated or delayed, depending on the circulating current state of the JPM. This fluxon delay can then be converted to an SFQ logic signal resulting in a digital qubit readout with a proximal microfabricated device, paving the way for cryogenic digital feedback necessary for error-correcting codes.
AB - As superconducting quantum processors increase in size and complexity, the scalability of standard techniques for qubit control and readout becomes a limiting factor. Replacing room temperature analog components with cryogenic digital components could allow for the realization of systems well beyond the current state-of-The-Art qubit arrays with tens of qubits. The standard technique for performing a qubit measurement with heterodyne readout uses a quantum-limited cryogenic amplifier chain and requires bulky microwave components inside the refrigerator with multiple control lines and pump signals. Additionally, the result is only accessible in software at room temperature. An alternative method for measuring qubits involves mapping the qubit state onto the photon occupation in a microwave cavity, followed by subsequent photon detection using a Josephson photomultiplier (JPM). The JPM measures the qubit and stores the result in a classical circulating current. To make use of this result, we can leverage existing single flux quantum (SFQ) circuitry. An underdamped Josephson transmission line (JTL) can be coupled to the JPM and fluxons traveling along the JTL are accelerated or delayed, depending on the circulating current state of the JPM. This fluxon delay can then be converted to an SFQ logic signal resulting in a digital qubit readout with a proximal microfabricated device, paving the way for cryogenic digital feedback necessary for error-correcting codes.
KW - Josephson junctions
KW - Superconducting devices
KW - superconducting integrated circuits
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U2 - 10.1109/TASC.2019.2908884
DO - 10.1109/TASC.2019.2908884
M3 - Article
AN - SCOPUS:85065990323
SN - 1051-8223
VL - 29
JO - IEEE Transactions on Applied Superconductivity
JF - IEEE Transactions on Applied Superconductivity
IS - 5
M1 - 8680055
ER -