The quantum Rabi model(QRM) is the simplest and most fundamental model that de scribes the quantum light-matter interactions. However, because the coupling strength is much smaller than the atomic frequencies, the anti Janyes-Cumming(JC) term is often...
The quantum Rabi model(QRM) is the simplest and most fundamental model that de scribes the quantum light-matter interactions. However, because the coupling strength is much smaller than the atomic frequencies, the anti Janyes-Cumming(JC) term is often neglected, making it challenging to experimentally realize the model’s full rich ness. Recently, quantum simulation techniques using trapped ions, photonic wave guide system, and circuit QED have enabled the study of various physical phenomena of the QRM. In this work, we study the generalized resonant Rabi model (GRRM), a variant of the quantum Rabi model that exhibits nontrivial topological properties. In the GRRM, the JC and anti-JC couplings are treated independently, and both bosonic and spin frequencies are set to zero. This model exhibits parity symmetry, ˆ Π=eiˆ a†ˆ aˆ σz, which divides the Hilbert space into two decoupled parity chains, analogous to the Su–Schrieffer–Heeger (SSH) model. Using a trapped-ion quantum simulator, we realize the GRRM and prepare its topological edge state via adiabatic state preparation. The edge state, identified as a squeezed vacuum, is characterized by quadrature measurements and phonon-number distribution. Our results confirm squeezing, even-parity Fock state composition, and exponential localization—all signatures of a topological edge state