Dynamic properties of atomic collective decay in cavity quantum electrodynamics<xref rid="cpb_27_12_124206fn1" ref-type="fn">*</xref><fn id="cpb_27_12_124206fn1"><label>*</label><p>Project supported by the National Natural Science Foundation of China (Grant Nos. 11504272, 11774262, 11474003, and 11504003), the National Key Basic Research Special Foundation (Grant No. 2016YFA0302800), the Joint Fund of the National Natural Science Foundation of China (Grant No. U1330203), the Fund from the Shanghai Science and Technology Committee (STCSM) (Grant No. 18JC1410900), and the Natural Science Foundation of Anhui Province, China (Grant Nos. 1408085MA19 and 1608085ME102).</p></fn>

Dynamic properties of atomic collective decay in cavity quantum electrodynamics**

Project supported by the National Natural Science Foundation of China (Grant Nos. 11504272, 11774262, 11474003, and 11504003), the National Key Basic Research Special Foundation (Grant No. 2016YFA0302800), the Joint Fund of the National Natural Science Foundation of China (Grant No. U1330203), the Fund from the Shanghai Science and Technology Committee (STCSM) (Grant No. 18JC1410900), and the Natural Science Foundation of Anhui Province, China (Grant Nos. 1408085MA19 and 1608085ME102).

Han Yu-Feng^{1, 2}, Zhu Cheng-Jie^{1, †}, Huang Xian-Shan², Yang Ya-Ping^{1, ‡}

(color online) The populations in states |eg〉 [panels (a) and (c)] and |ge〉 [panels (b) and (d)] with initial conditions of P_eg(0) = 1 and P_ge(0) = 0. Here, ϕ_z = 0 for the top two panels, but ϕ_z = π/2 for the button ones. The coupling strength is chosen as g₀ = 0.01 (blue curve), g₀ = 1 (green curve), and g₀ = 10 (red solid curve). Other system parameters are the same as those in Fig. 2.