Core Concepts
Quantum steering in coupled harmonic oscillators is highly sensitive to coupling strength, excitation levels, and resonance conditions, exhibiting distinct asymmetric behavior and diverging from previous weak-coupling approximations, particularly in the ultra-strong coupling regime.
Stats
For weak coupling (ϵ = 0.05), entanglement increases with quantum numbers n and m, while the ground state remains separable with linear entropy (SL) close to 0.
In the ultra-strong coupling regime (ϵ = 0.9), both ground and excited states exhibit entanglement, with higher excitation levels leading to stronger entanglement.
At resonance (ωx = ωy), Makarov's approximation predicts no dependence of linear entropy on coupling strength (ϵ), contradicting the exact results.
Makarov's model also incorrectly predicts a separable ground state (SM(0, 0) = 0) for all coupling strengths, contradicting established findings.
Discrepancies between Makarov's approximation and exact results are particularly pronounced for smaller quantum numbers and in the ultra-strong coupling regime.
In the weak coupling regime, quantum steering is only possible when one oscillator is excited (n ≠ 0 or m ≠ 0) and the other is in the ground state (m = 0 or n = 0).
Steering quantifiers in the weak coupling regime show a discrete increase with quantum numbers, separated by a fixed value.
At resonance (µ = 1) and in the decoupled case (µ = 0), quantum steering vanishes completely.
Ultra-strong coupling suppresses steering between weakly excited states.
Small frequency detuning from resonance can revive quantum steering.
Asymmetry in steering is observed, with one direction often dominating.