2021
DOI: 10.1016/j.physe.2021.114663
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Theory of nonlinear microwave absorption in an electron-doped and gapped graphene monolayer

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Cited by 1 publication
(2 citation statements)
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“…As we shall see further, we need to know both the linear surface conductivity σ (1) (ω) and the third-order nonlinear surface conductivity σ (3) (ω) ≡ σ (3) (−3ω; ω, ω, ω) in order to calculate the intensity of the third harmonic radiation generated in the reflected direction when the phosphorene layer is deposited on a dielectric substrate, such as SiO 2 . In deriving explicit expressions for those conductivities, we rely on the perturbative approach that we have used in our previous papers [45][46][47][48][49] dealing with graphene. Within the framework of the approach, equation ( 10) is solved iteratively in powers of the electric field amplitude E 0 up to the third order in E 0 .…”
Section: Theorymentioning
confidence: 99%
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“…As we shall see further, we need to know both the linear surface conductivity σ (1) (ω) and the third-order nonlinear surface conductivity σ (3) (ω) ≡ σ (3) (−3ω; ω, ω, ω) in order to calculate the intensity of the third harmonic radiation generated in the reflected direction when the phosphorene layer is deposited on a dielectric substrate, such as SiO 2 . In deriving explicit expressions for those conductivities, we rely on the perturbative approach that we have used in our previous papers [45][46][47][48][49] dealing with graphene. Within the framework of the approach, equation ( 10) is solved iteratively in powers of the electric field amplitude E 0 up to the third order in E 0 .…”
Section: Theorymentioning
confidence: 99%
“…[13]). In this case, as in the case of an electron-doped and gapped graphene monolayer [45][46][47][48][49], free mobile carriers can cause a substantial nonlinear microwave response of phosphorene due to its non-parabolic conduction band [50].…”
Section: Introductionmentioning
confidence: 99%