2021
DOI: 10.1063/5.0049678
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Generation of half-integer harmonics and efficient THz-to-visible frequency conversion in strained graphene

Abstract: We study the generation of harmonics from graphene under the influence of an artificial magnetic field, generated via bending of a graphene flake. We show how the Landau level structure induced by the pseudomagnetic field breaks the centrosymmetry of graphene, thus allowing the generation of even harmonics. We also show that depending on the impinging pulse duration, the nonlinear signal does not only contain the integer harmonics of the impinging pulse but also its half-integer ones due to the peculiar square… Show more

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Cited by 9 publications
(7 citation statements)
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“…Rectangular graphene flakes either free [42] or subjected to planar bending [43] have been analysed in the literature. Conical graphene rings in a magnetic field have also been studied, but only in the continuum limit approximation in the vicinity of the Dirac points and very far from the vertex [44,45].…”
Section: Introductionmentioning
confidence: 99%
“…Rectangular graphene flakes either free [42] or subjected to planar bending [43] have been analysed in the literature. Conical graphene rings in a magnetic field have also been studied, but only in the continuum limit approximation in the vicinity of the Dirac points and very far from the vertex [44,45].…”
Section: Introductionmentioning
confidence: 99%
“…Assuming a strain profile as the one described in Ref. 33, and pictorially represented in Fig. 2, we obtain an AGF A (s) = −B y x, corresponding to a uniform magnetic field oriented perpendicular to the graphene plane, i.e., B = B ẑ.…”
Section: Bent Graphene In the Presence Of Socmentioning
confidence: 99%
“…n ∈ N 0 indicates the Landau levels in the conduction (α = 1) and valence (α = −1) band, respectively. Notice, moreover, that since the total Hamiltonian factors in spin space, there cannot be a common n = 0 Landau level, as in the case of no intrinsic SOC [33], but rather two separate levels, with spin-dependent eigenvalues E 0,β = −β(∆ I − ∆ Z ), and spin-polarized eigenstates…”
Section: A Instantaneous Eigenstates Of ĥξ Tot For Intrinsic Soc Onlymentioning
confidence: 99%
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