At the dawn of the 21st century, the solid-state analogue of the interaction between atom and light in a superconducting system was theoretically proposed by Yu. Makhilin, G. Schön, and A. Shnirman [Rev. Mod. Phys. 73 (2001) 357] and by F. Marquardt and C. Bruder [Phys. Rev. B 63 (2001) 054514]. It has been experimentally demonstrated by I. Chiorescu, et al. [Nature 431 (2004) 159] and by A. Wallraff, et al. [Nature 431 (2004) 162]. In that solid-state analogue, an artificial atom and a microwave are used respectively for the atom and the light. The interaction is made near a microwave resonator on a superconducting circuit. Here, the artificial atom is made by using a superconducting LC circuit. The harmonic oscillator atom is obtained in the case without any Josephson junction, and the 2-level atom is based on the anharmonicity coming from Josephson junctions. Their current cutting-edge technology is beginning to show us the ultra-strong coupling regime of the atom-light interaction beyond its standard regime of quantum electrodynamics. For instance, F. Yoshihara, et al. have demonstrated around 100% of the atom-light interaction in their experiment [Nature Physics 13 (2017) 44]. I would like to introduce the following subjects on quantum simulation using the artificial atom on the superconducting circuit. I chiefly talk about