Figure 6From: A similarity of quantum phase transition and quench dynamics in the Dicke model beyond the thermodynamic limitErrors of solutions from the effective Hamiltonian of Eq. (a5) with the numerical solutions at \(g=\frac{1}{2}\) [(a)–(d)] and \(g=1\) [(e)–(h)]. At the top-right corner of each subgraph, the detail between the error and \(\varOmega/w_{0}\) is magnified when \(N=10\)Back to article page