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The Tavis-Cummings model is a quantum optical theoretical system describing an ensemble of identical two-level atoms coupled symmetrically to a single-mode quantized bosonic field[1]. The Tavis-Cummings model extends the Jaynes-Cummings model to larger spin-numbers representing collections of multiple atoms, and differs from the Dicke model in its use of the rotating-wave approximation to conserve the system's total number of excitations. Originally modeled by Michael Tavis and Fred Cummings to unify representations of atomic gases in electromagnetic fields under a single fully quantum Hamiltonian, as Robert Dicke had done previously using perturbation theory, the Tavis-Cummings model's restriction to a single field-mode with negligible counterrotating interactions simplifies the system's mathematics while preserving the breadth of its dynamics. The Tavis-Cummings model demonstrates superradiance[2], bright and dark states[3], Rabi oscillations and spontaneous emission, and other features of interest in quantum electrodynamics, quantum control and computation, atomic and molecular physics, and many-body physics[4]. The model has been experimentally tested to determine the conditions of its viability[5][6], and realized in semiconducting[7] and superconducting qubits[2][3].
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