Nb-based Josephson parametric amplifier for superconducting qubit measurement<xref rid="cpb_28_11_110303fn1" ref-type="fn">*</xref><fn id="cpb_28_11_110303fn1"><label>*</label><p>Project supported by the Science Funds from the Ministry of Science and Technology of China (Grant Nos. 2015CB921104 and 2016YFA0300601), the National Natural Science Foundation of China (Grant Nos. 11674380 and 11874063), the Strategic Priority Research Program of the Chinese Academy of Sciences (Grant Nos. XDB07010300 and XDB28000000), and the Key Research and Development Program of Guangdong Province, China (Grant No. 2018B030326001).</p></fn>

Nb-based Josephson parametric amplifier for superconducting qubit measurement**

Project supported by the Science Funds from the Ministry of Science and Technology of China (Grant Nos. 2015CB921104 and 2016YFA0300601), the National Natural Science Foundation of China (Grant Nos. 11674380 and 11874063), the Strategic Priority Research Program of the Chinese Academy of Sciences (Grant Nos. XDB07010300 and XDB28000000), and the Key Research and Development Program of Guangdong Province, China (Grant No. 2018B030326001).

Su Fei-Fan^{1, 2}, Wang Zi-Ting^{1, 2}, Xu Hui-Kai^{1, 2}, Zhao Shou-Kuan^{1, 2}, Yan Hai-Sheng^{1, 2}, Yang Zhao-Hua^{1, 2}, Tian Ye^{1, 2}, Zhao Shi-Ping^{1, 2, 3, †}

The signal frequency dependence of the gain (a) and noise (b). Solid line and dots: I_b = −0.055 mA, P = −31.9 dBm; dashed line and crosses: I_b = 0.54 mA, P = −32.5 dBm. The two parameter sets are indicated in Fig. 4(a) as left and right white dots, respectively, with the other parameters used in the figure unchanged.