Table 1 Extracted and derived transmon parameters

From: Nearly quantum-limited microwave amplification via interfering degenerate stimulated emission in a single artificial atom

EC/h

EJ/h

EJ/EC

ω10/2π

ω21/2π

ω32/2π

ω43/2π

Γ10/2π

\({\Gamma }_{1}^{\phi }/2\pi\)

γ10/2π

[MHz]

[GHz]

[GHz]

[GHz]

[GHz]

[GHz]

[MHz]

[MHz]

[MHz]

228

13.67

59.96

4.766

4.538

4.287

4.005

2.264

0.0317

1.164

  1. We extract the transition frequency ω10, the relaxation rate Γ10, and the decoherence rate γ10 by fitting the magnitude and phase data from single-tone scattering (see Supplementary Information Fig. 2b)34. We calculate the pure dephasing rate \({\Gamma }_{1}^{\phi }\) from Γ10 and γ10, using γ10 = \({\Gamma }_{10}/2+{\Gamma }_{1}^{\phi }\). From the four-tone spectroscopy (see Supplementary Information Fig. 2d), we extract ω21, ω32, and ω43, and the anharmonicity between the \(\left\vert 0\right\rangle \leftrightarrow \left\vert 1\right\rangle\) transition and the \(\left\vert 1\right\rangle \leftrightarrow \left\vert 2\right\rangle\) transition. The anharmonicity approximately equals the charging energy24EC. We calculate the Josephson energy EJ and EJ/EC from ω10 and EC, where \(\hslash {\omega }_{10}\simeq \sqrt{8{E}_{{\rm {J}}}{E}_{{\rm {C}}}}-{E}_{{\rm {C}}}\).