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We rewrite the interaction part of the Hamiltonian as follows ˆHint =− NX k=1 ˆσ(k) x ⊗ h d(k) eg · ˆE+(rk) + h.c

Direct construction of a single hybrid continuum Instead of the orthogonalization of the bright modes operators of the e-, m-continua separately, one can introduce a bright oper

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Quantum plasmonics with N emitters: bright hybrid continuum selection

quant-ph · 2026-04-23 · unverdicted · novelty 6.0

For N quantum emitters coupled to a plasmon-polariton field supported by a finite dielectric, the interacting continuum reduces exactly to N non-degenerate one-dimensional hybrid continua, matching the macroscopic Langevin model through cancellation in the coupling and Green tensor.

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  • Quantum plasmonics with N emitters: bright hybrid continuum selection quant-ph · 2026-04-23 · unverdicted · none · ref 7

    For N quantum emitters coupled to a plasmon-polariton field supported by a finite dielectric, the interacting continuum reduces exactly to N non-degenerate one-dimensional hybrid continua, matching the macroscopic Langevin model through cancellation in the coupling and Green tensor.