2017
DOI: 10.1364/optica.4.000595
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Universal description of channel plasmons in two-dimensional materials

Abstract: Channeling surface plasmon-polaritons to control their propagation direction is of the utmost importance for future optoelectronic devices. Here, we develop an effective-index method to describe and characterize the properties of 2D material's channel plasmon-polaritons (CPPs) guided along a V-shaped channel. Focusing on the case of graphene, we derive a universal Schrödinger-like equation from which one can determine the dispersion relation of graphene CPPs and corresponding field distributions at any given f… Show more

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Cited by 14 publications
(16 citation statements)
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“…3a ). It is notable that the field intensity distribution profiles in the apex and valley regions are different because of the broken symmetry of the plasmonic resonance modes between the apex and valley due to the undulating subtrate 9 , 36 . The σ ext and quality factor ( Q -factor) were enhanced approximately twofold for the undulating substrate compared to the free-standing crumpled graphene (14.0 vs. 7.6% and 63.8 vs. 26.1) (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…3a ). It is notable that the field intensity distribution profiles in the apex and valley regions are different because of the broken symmetry of the plasmonic resonance modes between the apex and valley due to the undulating subtrate 9 , 36 . The σ ext and quality factor ( Q -factor) were enhanced approximately twofold for the undulating substrate compared to the free-standing crumpled graphene (14.0 vs. 7.6% and 63.8 vs. 26.1) (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Moreover, owing to the extreme subwavelength confinement promoted by GPs, the nonretarded limit (defined by the absence of retardation effects) can be taken without any loss of accuracy in nearly all the relevant scenarios. In fact, treating plasmons in graphene within a nonretarded approach often constitutes an excellent approximation, as demonstrated in a number of works . In this vein, we take the nonretarded limit (i.e., q ≫ k 0 ) of Equation , thereby obtaining the nonretarded dispersion relation of graphene plasmons q=2iωε0ε¯σ(q,ω) where we have introduced the quantity ε¯=(ε1+ε2)/2 without loss of generality .…”
Section: Graphene Plasmon Polaritonsmentioning
confidence: 99%
“…After investigating MPs in flat structures of monolayer BP, we now consider a nonplanar geometry in which the BP monolayer is folded into a wedge structure forming a triangular channel [21,22,25]. Compared to the plane and edge structures, a wedge structure composed of a 2D material provides a flexible way to tune the plasmon mode by the external magnetic field because the two wedge arms exhibit different responses for a given external magnetic field.…”
mentioning
confidence: 99%