[1] Rabi I I. Space quantization in a gyrating magnetic field[J]. Phys Rev, 1937, 51(8): 652-654.
[2] Jaynes E T, Cummings F W. Comparison of quantum and semiclassical radiation theories with application to the beam maser[J]. Proc IEEE, 1963, 51(1): 89-109.
[3] Leibfried D, Blatt R, Monroe C, et al.. Quantum dynamics of single trapped ions[J]. Rev Mod Phys, 2003, 75(1): 281-324.
[4] Holstein T. Studies of polaron motion: Part I. The molecular-crystal model[J]. Ann Phys, 1959, 8(3): 325-342.
[5] Balázs D, Klaus Z, Peter T, et al.. Rabi oscillations in iandau-quantized graphene[J]. Phys Rev Lett, 2009, 102(3): 036803.
[6] Kibis O V. Metal-insulator transition in graphene induced by circularly polarized photons[J]. Phys Rev B, 2009, 81(16): 165433.
[7] Peter E, Senellart P, Martrou D, et al.. Exciton photon strong-coupling regime for a single quantum dot in a microcavity[J]. Phys Rev Lett, 2004, 95(6): 067401.
[8] Hennessy K, Badolato A, Winger M, et al.. Quantum nature of a strongly-coupled single quantum dot-cavity system[J]. Nature, 2006, 445(7130): 896-899.
[9] Son W, Kim M S, Lee J, et al.. Entanglement transfer from continuous variables to qubits[J]. J Mod Opt, 2002, 49(10): 1739-1746.
[10] Kraus B, Cirac J I. Discrete entanglement distribution with squeezed light[J]. Phys Rev Lett, 2004, 92(1): 013602.
[11] Paternostro M, Son W, Kim M S. Complete conditions for entanglement transfer[J]. Phys Rev Lett, 2004, 92(19): 197901.
[12] Paternostro M, Son W, Kim M S, et al.. Dynamical entanglement transfer for quantum-information networks[J]. Phys Rev A, 2004, 70(2): 022320.
[13] Lee J, Paternostro M, Kim M S, et al.. Entanglement reciprocation between qubits and continuous variables[J]. Phys Rev Lett, 2006, 96(8): 080501.
[14] Zhou L, Yang G H. Entanglement reciprocation between atomic qubits and an entangled coherent state[J]. J Phys B, 2006, 39(24): 5143-5150.
[15] Rendell R W, Rajagopal A K. Revivals and entanglement from initially entangled mixed states of a damped Jaynes-Cummings model[J]. Phys Rev A, 2003, 67(6): 062110.
[16] Ynac M, Eberly J H. Coherent-state control of noninteracting quantum entanglement[J]. Phys Rev A, 2010, 82(2): 022321.
[17] You J Q, Nori F. Superconducting circuits and quantum information[J]. Phys Today, 2006, 58(11): 42-47.
[18] You J Q, Franco N. Atomic physics and quantum optics using superconducting circuits[J]. Nature, 2011, 474(7353): 589-597.
[19] Nation P D, Johansson J R, Blencowe M P, et al.. Colloquium: Stimulating uncertainty: Amplifying the quantum vacuum with superconducting circuits[J]. Rev Mod Phys, 2012, 84(1): 1-24.
[20] Xiang Z L, Ashhab S, You J Q, et al.. Hybrid quantum circuits: Superconducting circuits interacting with other quantum systems[J]. Rev Mod Phys, 2013, 85(1): 623-653.
[21] Cao X, You J Q, Zheng H, et al.. A qubit strongly coupled to a resonant cavity: Asymmetry of the spontaneous emission spectrum beyond the rotating wave approximation[J]. New J Phys, 2011, 13(7): 073002.
[22] Cao X F, You J Q, Zheng H, et al.. Dynamics and quantum Zeno effect for a qubit in either a low- or high-frequency bath beyond the rotating-wave approximation[J]. Phys Rev A, 2010, 82(2): 022119.
[23] Cao X, Ai Q, Sun C P, et al.. The transition from quantum Zeno to anti-Zeno effects for a qubit in a cavity by varying the cavity frequency[J]. Phys Lett A, 2012, 376(4): 349-357.
[24] Lü X Y, Ashhab S, Cui W, et al.. Two-qubit gate operations in superconducting circuits with strong coupling and weak anharmonicity[J]. New J Phys, 2012, 14(7): 073041.
[25] Hu X, Liu Y X, Nori F. Strong coupling of a spin qubit to a superconducting stripline cavity[J]. Phys Rev B, 2012, 86(3): 035314.
[26] Chen Q H, Li L, Liu T. The spectrum in qubit-oscillator systems in the ultrastrong coupling regime[J]. Chin Phys Lett, 2012, 29(1): 014208.
[27] Walther H, Varcoe B T H, Englert B G, et al.. Cavity quantum electrodynamics[J]. Rep Prog Phys, 2006, 69(5): 1325-1382.
[28] Günter G, Anappara A A, Hees J, et al.. Sub-cycle switch-on of ultrastrong light-matter interaction[J]. Nature, 2009, 458(7235): 178-181.
[29] Niemczyk T, Deppe F, Huebl H, et al.. Circuit quantum electrodynamics in the ultrastrong-coupling regime[J]. Nat Phys, 2010, 6(10): 772-776.
[30] Casanova J, Romero G, Lizuain I, et al.. Deep strong coupling regime of the Jaynes-Cummings model[J]. Phys Rev Lett, 2010, 105(26): 263603.
[31] Ballester D, Romero G, García-Ripoll J J, et al.. Quantum simulation of the ultrastrong coupling dynamics in circuit QED[J]. Phys Rev X, 2012, 2(2): 021007.
[32] Romero G, Ballester D, Wang Y M, et al.. Ultrafast quantum gates in circuit QED[J]. Phys Rev Lett, 2012, 108(12): 120501.
[33] He S, Wang C, Chen Q H, et al.. First-order corrections to the rotating-wave approximation in the Jaynes-Cummings model[J]. Phys Rev A, 2012, 86(3): 033837.
[34] Wolf F A, Vallone F, Romero G, et al.. Dynamical correlation functions and the quantum Rabi model[J]. Phys Rev A, 2013, 87(2): 023835.
[35] Ping Y T, Lovett B W, Benjamin S C, et al.. Practicality of spin chain wiring in diamond quantum technologies[J]. Phys Rev Lett, 2013, 110(10): 100503.
[36] Yoshihara F, Nakamura Y, Yan F, et al.. Flux qubit noise spectroscopy using Rabi oscillations under strong driving conditions[J]. Phys Rev B, 2014, 89(2): 020503.
[37] Irish E K, Gea-Banacloche G. Oscillator tunneling dynamics in the Rabi model[J]. Phys Rev B, 2014, 89(8): 085421.
[38] Sete E A, Eleuch H. High-efficiency quantum state transfer and quantum memory using a mechanical oscillator[J]. Phys Rev A, 2015, 91(3): 032309.
[39] Yan Y, Lü Z, Zheng H. Bloch-Siegert shift of the Rabi model[J]. Phys Rev A, 2015, 91(5): 053834.
[40] Kibis O V, Ya S G, Maksimenko S A, et al.. Matter coupling to strong electromagnetic fields in two-level quantum systems with broken inversion symmetry[J]. Phys Rev Lett, 2009, 102(2): 023601.
[41] Avetissian H K, Avchyan B R, Mkrtchian G F. Tunable high-power terahertz radiation generation in three-level atomic and molecular systems[J]. Phys Rev A, 2010, 82(6): 063412.
[42] Avetissian H K, Avchyan B R, Mkrtchian G F. Efficient generation of moderately high harmonics by multiphoton resonant excitation of atoms[J]. Phys Rev A, 2008, 77(2): 023409.
[43] Avetissian H K, Avchyan B R, Mkrtchian G F. Coherent radiation by two-level quantum systems with permanent dipole moments under multiphoton resonant laser excitation[J]. J Phys B, 2012, 45(2): 025402.
[44] Avetissian H K, Mkrtchian G F. Two-level system with broken inversion symmetry coupled to a quantum harmonic oscillator[J]. Phys Rev A, 2013, 88(4): 043811.
[45] Balandin A, Wang K L. Feasibility study of the quantum XOR gate based on coupled asymmetric semiconductor quantum dots[J]. Superlattices Microstruct, 1999, 25(3): 509-518.
[46] Blais A, Huang R S, Wallraff A, et al.. Cavity quantum electrodynamics for superconducting electrical circuits: An architecture for quantum computation[J]. Phys Rev A, 2004, 69(6): 062320.
[48] Guo Zhanying, Zhang Xinhai, Xiao Ruihua, et al.. Dynamics of quantum entanglement in a two-qubit XXZ Heisenberg system[J]. Acta Optica Sinica, 2014, 34(7): 0727001.
[49] Zhai Shuqin, Yang Rui. Three-color and tripartite entangled state from cascaded type I second-harmonic generations[J]. Acta Optica Sinica, 2014, 34(4): 0427002.
[50] You J Q, Tsai J S, Nori F. Controllable manipulation and entanglement of macroscopic quantum states in coupled charge qubits[J]. Phys Rev B, 2003, 68(2): 024510.
[51] You J Q, Franco N. Atomic physics and quantum optics using superconducting circuits[J]. Nature, 2011, 474(7353): 589-597.
[52] Wallquist M, Hammerer K, Rabl P, et al.. Hybrid quantum devices and quantum engineering[J]. Phys Scripta, 2009, T137: 014001.
[53] Wallraff A, Schuster D I, Blais A, et al.. Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics[J]. Nature, 2004, 431(7005): 162-167.