Theory of plasmonic effects in nonlinear optics: the case of graphene
arXiv:1610.04854 · doi:10.1103/PhysRevB.95.035416
Abstract
We develop a microscopic large- theory of electron-electron interaction corrections to multi-legged Feynman diagrams describing second- and third-order nonlinear response functions. Our theory, which reduces to the well-known random phase approximation in the linear-response limit, is completely general and is useful to understand all second- and third-order nonlinear effects, including harmonic generation, wave mixing, and photon drag. We apply our theoretical framework to the case of graphene, by carrying out microscopic calculations of the second- and third-order nonlinear response functions of an interacting two-dimensional (2D) gas of massless Dirac fermions. We compare our results with recent measurements, where all-optical launching of graphene plasmons has been achieved by virtue of the finiteness of the quasi-homogeneous second-order nonlinear response of this inversion-symmetric 2D material.
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- Cyclotron resonance overtones and near-field magnetoabsorption via terahertz Bernstein modes in graphene
- Roadmap on Nonlocality in Photonic Materials and Metamaterials
- Quantized Nonlinear Conductance in Ballistic Metals
- Gauge invariance and Ward identities in nonlinear response theory
- Nonlinear Density Response and Higher Order Correlation Functions in Warm Dense Matter
- Analysis of dynamical effects in the uniform electron liquids with the self-consistent method of moments complemented by the Shannon information entropy and the path-integral Monte-Carlo simulations
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- Graphene as a source of entangled plasmons
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- Many-Body Effects in Third Harmonic Generation of Graphene
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- Plasmon polariton assisted second-harmonic generation in graphene
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