Accurate phase‑boundary predictions accelerate the design of cavity‑QED devices and quantum simulators, directly impacting emerging quantum technologies.
The combination of numerical linked‑cluster expansions (NLCE) with density‑matrix renormalization‑group (DMRG) calculations marks a methodological leap for one‑dimensional light‑matter systems. By mapping the Dicke‑Ising chain onto a self‑consistent effective matter Hamiltonian, the photon field is absorbed as a static background, eliminating the need to track photon‑spin entanglement. This simplification allows NLCE to capture extensive cluster contributions while DMRG solves the resulting many‑body Hamiltonian with high fidelity. The hybrid approach delivers unprecedented numerical stability and scales efficiently, opening a practical pathway for tackling other strongly coupled cavity‑QED models.
The refined calculations pinpoint the multicritical point of the ferromagnetic Dicke‑Ising chain with a relative precision of 10⁻⁴, far surpassing earlier estimates. For antiferromagnetic couplings the method confirms a narrow superradiant phase that had only been conjectured, identifying it as the ground state of an antiferromagnetic transverse‑field Ising model subjected to a longitudinal field. The study also elucidates the continuous polariton‑condensation that initiates this phase, followed by a first‑order transition into a paramagnetic superradiant regime. These insights resolve long‑standing ambiguities in the model’s phase diagram.
Beyond its immediate scientific merit, the NLCE + DMRG framework equips experimental groups with a reliable predictive tool for designing cavity‑QED and circuit‑QED platforms. Accurate knowledge of phase boundaries enables deterministic preparation of desired quantum states, a prerequisite for scalable quantum simulators and error‑resilient quantum sensing. Moreover, the self‑consistent Hamiltonian mapping can be extended to higher dimensions or to systems with long‑range interactions, promising further breakthroughs in engineered quantum materials. As the field moves toward integrated photonic‑matter architectures, such computational precision will be essential for bridging theory and hardware.
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