2019
DOI: 10.1364/josab.36.000200
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Strong tunable photomixing in semi-Dirac materials in the terahertz regime

Abstract: We demonstrate a strong and anisotropic photomixing effect in an electronic system whose energy-momentum dispersion is parabolic in the ? direction and linear in the ? direction, such as a TiO 2 /VO 2 multilayered structure. The third-order photoresponses along the linear and parabolic directions have been analyzed and determined quantitatively. We have found a remarkable tunability of the mixing efficiency along the parabolic direction by a small electric field in the linear direction, up to two orders of mag… Show more

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Cited by 7 publications
(3 citation statements)
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References 21 publications
(18 reference statements)
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“…In the low-energy limit, the electrons in these exotic materials obey relativistic, Diraclike Hamiltonians. Their pseudo-massless particle behavior confers these materials unique optical properties such as high electromagnetic field confinement [1][2][3][4] and strong optical nonlinearity, [5][6][7][8][9][10][11][12][13][14][15][16] making them desirable for uses like tabletop generation of high-brightness coherent radiation spanning from the x-ray to the terahertz regimes through mechanisms such as free-electron-graphene plasmon scattering, [17,18] highharmonic generation, [19][20][21][22] and transition radiation, [23] and also as saturable absorbers for infrared ultrafast lasers. [24][25][26][27] Recently, a new class of quantum materials which behave like the bulk analogues of graphene have also attracted significant attention -3D Dirac semimetals (DSMs).…”
Section: Introductionmentioning
confidence: 99%
“…In the low-energy limit, the electrons in these exotic materials obey relativistic, Diraclike Hamiltonians. Their pseudo-massless particle behavior confers these materials unique optical properties such as high electromagnetic field confinement [1][2][3][4] and strong optical nonlinearity, [5][6][7][8][9][10][11][12][13][14][15][16] making them desirable for uses like tabletop generation of high-brightness coherent radiation spanning from the x-ray to the terahertz regimes through mechanisms such as free-electron-graphene plasmon scattering, [17,18] highharmonic generation, [19][20][21][22] and transition radiation, [23] and also as saturable absorbers for infrared ultrafast lasers. [24][25][26][27] Recently, a new class of quantum materials which behave like the bulk analogues of graphene have also attracted significant attention -3D Dirac semimetals (DSMs).…”
Section: Introductionmentioning
confidence: 99%
“…The formation of the polaron (or even the trion) and the polariton have been realized in semiconductor heterostructure by using the technique of cavity coupling in the presence of exciton-electron interactions [22,23]. For semi-Dirac system, which has very interesting electronic and topological properties under irradiation [24,25,26], although its anisotropic dispersion, we can still approximate it as the one similar to the twodimensional electron gas when the carrier density is just slightly larger than the band gap (D ≫ µ ↑ − D > 0) and with small momentum. In the mean time, the chemical potential of the impurity can be treated as a negative unphysical parameter µ ↓ < −µ ↑ during the calculation of the polaron energy (i.e., the pole of the dressed Green's function).…”
Section: Introductionmentioning
confidence: 99%
“…The formation of the polaron (or even the trion) and the polariton have been realized in semiconductor heterostructure by using the technique of cavity coupling in the presence of exciton-electron interactions [24,25]. For semi-Dirac system, which has very interesting electronic and topological properties under irradiation [26][27][28], although its anisotropic dispersion, we can still approximate it as the one similar to the 2D electron gas when the carrier density is just slightly larger than the band gap ( m ->  D D 0 …”
Section: Introductionmentioning
confidence: 99%