Fig. 3: Residual \(\left|e\right\rangle\) state population measurement and improvement of the readout fidelity. | Nature Communications

Fig. 3: Residual \(\left|e\right\rangle\) state population measurement and improvement of the readout fidelity.

From: Rapid and unconditional parametric reset protocol for tunable superconducting qubits

Fig. 3

a Residual \(\left|e\right\rangle\) population measurement with Reference (red) and Signal (blue) Rabi oscillations with solid sinusoidal fitting curves. From the fitting, two Rabi amplitudes(Asig and Aref) can be extracted. The Reference and Signal pulse sequences are shown in the upper left corner. P1 and P2 are two measured points in b. b \(\left|e\right\rangle\) population measurement with different parametric reset pulse duration τ. Each data point is acquired by a "two-point method" described in the main text. At 34 ns, the population of the \(\left|e\right\rangle\) decays to the first minimum value 0.08 ± 0.08% and remains below 0.1% after 1000 ns. The error bars are statistical ( ± 1 s.d.) with 50 repetitions. c Readout fidelity enhancement with the 34 ns parametric reset pulse. The circles (squares) display the IQ analysis with (without) the 34 ns parametric pulse. Both \(\left|g\right\rangle\) (blue) and \(\left|e\right\rangle\) (red) are prepared and measured. When preparing the \(\left|g\right\rangle\) state, the residual \(\left|e\right\rangle\) state population due to the thermal excitation decreases more than one order of magnitude after applying the parametric reset pulse. The readout fidelity consequently improves from 96.13% to 99.43% for \(\left|g\right\rangle\) and 92.69% to 96.05% for \(\left|e\right\rangle\) respectively.

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