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@ARTICLE{Ansari:902779,
author = {Ansari, Mohammad},
title = {{S}uperconducting qubits beyond the dispersive regime},
journal = {Physical review / B},
volume = {100},
number = {2},
issn = {1098-0121},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2021-04550},
pages = {024509},
year = {2019},
abstract = {Superconducting circuits consisting of a few low-anharmonic
transmons coupled to readout and bus resonators can perform
basic quantum computations. Since the number of qubits in
such circuits is limited to not more than a few tens, the
qubits can be designed to operate within the dispersive
regime where frequency detunings are much stronger than
coupling strengths. However, scaling up the number of qubits
will bring the circuit out of the regime, and this
invalidates current theories. We develop a formalism that
allows to consistently diagonalize the superconducting
circuit Hamiltonian beyond the dispersive regime. This will
allow to study qubit-qubit interaction unperturbatively,
therefore, our formalism remains valid and accurate at small
or even negligible frequency detuning; thus, our formalism
serves as a theoretical ground for designing qubit
characteristics for scaling up the number of qubits in
superconducting circuits. We study the most important
circuits with single- and two-qubit gates, i.e., a single
transmon coupled to a resonator and two transmons sharing a
bus resonator. Surprisingly, our formalism allows to
determine the circuit characteristics, such as dressed
frequencies and Kerr couplings, in closed-form formulas that
not only reproduce perturbative results, but also
extrapolate beyond the dispersive regime and can ultimately
reproduce (and even modify) the Jaynes-Cumming results at
resonant frequencies.},
cin = {PGI-2},
ddc = {530},
cid = {I:(DE-Juel1)PGI-2-20110106},
pnm = {5224 - Quantum Networking (POF4-522)},
pid = {G:(DE-HGF)POF4-5224},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000476685600003},
doi = {10.1103/PhysRevB.100.024509},
url = {https://juser.fz-juelich.de/record/902779},
}