2018
DOI: 10.1103/physreva.97.063836
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Nonlinear coupled-mode-theory framework for graphene-induced saturable absorption in nanophotonic resonant structures

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Cited by 17 publications
(21 citation statements)
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“…𝜏 𝑆𝐴 [36], where 𝜏 𝑒 and 𝜏 𝑆𝐴 are the photon resonator lifetimes corresponding to the coupling and resistive losses, respectively. The variable lifetime 𝜏 𝑆𝐴 depends on the energy in the cavity:…”
Section: )mentioning
confidence: 99%
“…𝜏 𝑆𝐴 [36], where 𝜏 𝑒 and 𝜏 𝑆𝐴 are the photon resonator lifetimes corresponding to the coupling and resistive losses, respectively. The variable lifetime 𝜏 𝑆𝐴 depends on the energy in the cavity:…”
Section: )mentioning
confidence: 99%
“…σ FCD is related to the FCD effect, γ FCA and α TPA is, respectively, the FCA absorption coefficient and TPA coefficient. W sat is the total energy stored in the cavity at the onset of saturable absorption [55,56]. τ f c is the normalized carrier lifetime, and n is the normalized carrier density.…”
Section: Mrr-based Photonic Neuronmentioning
confidence: 99%
“…Consequently, the optical response of graphene metasurfaces can be highly isotropic, when the geometry of graphene unit cell is symmetric. In fact, patterned graphene has already been employed in the design of terahertz devices, such as perfect absorbers, filters, and tunable reflectors [38][39][40][41][42][43] . In this context, a particularly appealing physical property of graphene is the tunability of its dielectric constant, a unique functionality that is highly relevant to the design of active photonic devices.…”
Section: Introductionmentioning
confidence: 99%