Plasmonics in graphene at infrared frequencies

By Marinko Jablan, Hrvoje Buljan, M. Soljavci'c. 2009

1,876 citations recorded by the source corpus.

We point out that plasmons in doped graphene simultaneously enable low-losses and significant wave localization for frequencies below that of the opti

Subfields: Biomedical Engineering, Electronic, Optical and Magnetic Materials, Materials Chemistry

View Paper: https://www.semanticscholar.org/paper/b6f27be10370fd0cd5153516946f37ef2ae15eed

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Citations in the corpus

Integral Equation Analysis of Plane Wave Scattering by Coplanar Graphene-Strip Gratings in the THz Range (2013, background): “Graphene is very interesting in view of possibility of strong interaction with electromagnetic waves in the THz frequency range [3], [4].”
Plasmonic photocatalysis (2013, background): “Achieving LSPR using these nanoparticles is delicate but possible [229].”
Graphene-Based Plasmonic Tunable Low-Pass Filters in the Terahertz Band (2013, background): “Currently, graphene-based plasmonic components ranging from waveguides [7]–[10], antennas [11]–[14], reflectarrays [15], amplifiers [16], switches [17], modulators [18], or phaseshifters [19] to sensors [20], [21] have already been proposed and investigated.”
Graphene-based Plasmonic Nano-Antenna for Terahertz Band Communication in Nanonetworks (2013, positive): “The majority of existing studies [6], [14], [17], [20] are focused on inﬁnitely large graphene sheets.”
Graphene-based nano-patch antenna for terahertz radiation (2012, neutral): “An infinite graphene layer placed on the air-dielectric interface supports transverse-magnetic (TM) SPP waves with a dispersion relation given by [5]”
Graphene-plasmon polaritons: From fundamental properties to potential applications (2016, neutral): “The condition for the transverse magnetic polarized field propagating in the plane can be described as [35, 51] ε √ k2 // − ε+ω2 c2 + ε− √ k2 // − ε−ω2 c2 = σ(k//, ω) iε0ω , (1)”
Graphene plasmon waveguiding and hybridization in individual and paired nanoribbons. (2012, background): “Equation 3 is obtained by expressing eq 1 (with χ = 1 for selfstanding ribbons) in terms of the plasmonwavelength, λp = 4π 2 Im{σ(ωp)}/ωp, which is in turn derived from the plasmon dispersion relation in homogeneous graphene k ) SP = iω/[2πσ(ω)].(18) Incidentally, the dispersion relationof thewavele”