31 research outputs found

    Molecular Beam Epitaxy Growth of Transition Metal Dichalcogenide (Mo,Mn)Se2_2 on 2D, 3D and polycrystalline substrates

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    Magnetic doping of 2D materials such as Transition Metal Dichalcogenides is promising for the enhancement of magneto-optical properties, as it was previously observed for 3D diluted magnetic semiconductors. To maximize the effect of magnetic ions, they should be incorporated into the crystal lattice of 2D material rather than form separated precipitates. This work shows a study on incorporating magnetic manganese ions into the MoSe2_2 monolayers using molecular beam epitaxy. We test growth on various substrates with very different properties: polycrystalline SiO2_2 on Si, exfoliated 2D hexagonal Boron Nitride flakes (placed on SiO2_2 / Si), monocrystalline sapphire, and exfoliated graphite (on tantalum foil). Although atomic force microscopy images indicate the presence of MnSe precipitates, but at the same time, various techniques reveal effects related to alloying MoSe2_2 with Mn: Raman scattering and photoluminescence measurements show energy shift related to the presence of Mn, scanning transmission microscopy shows Mn induced partial transformation of 1H to 1T^\prime phase. Above effects evidence partial incorporation of Mn into the MoSe2_2 layer.Comment: 13 pages, 8 figure

    Molecular Beam Epitaxy growth of MoTe2_{\tiny{\textrm{2}}} on Hexagonal Boron Nitride

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    Hexagonal boron nitride has already been proven to serve as a decent substrate for high quality epitaxial growth of several 2D materials, such as graphene, MoSe2_{\tiny{\textrm{2}}}, MoS2_{\tiny{\textrm{2}}} or WSe2_{\tiny{\textrm{2}}}. Here, we present for the first time the molecular beam epitaxy growth of MoTe2_{\tiny{\textrm{2}}} on atomically smooth hexagonal boron nitride (hBN) substrate. Occurrence of MoTe2_{\tiny{\textrm{2}}} in various crystalline phases such as distorted octahedral 1T' phase with semimetal properties or hexagonal 2H phase with semiconducting properties opens a possibility of realisation of crystal-phase homostructures with tunable properties. Atomic force microscopy studies of MoTe2_{\tiny{\textrm{2}}} grown in a single monolayer regime enable us to determine surface morphology as a function of the growth conditions. The diffusion constant of MoTe2_{\tiny{\textrm{2}}} grown on hBN can be altered 5 times by annealing after the growth, reaching about 5 ⋅\cdot 10−6^{-6} cm2^{2}/s. Raman spectroscopy results suggest a coexistence of both 2H and 1T' MoTe2_{\tiny{\textrm{2}}} phases in the studied samples.Comment: 6 pages, 3 figure

    Magneto-optical induced supermode switching in quantum fluids of light

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    The insensitivity of photons towards external magnetic fields forms one of the hardest barriers against efficient magneto-optical control, aiming at modulating the polarization state of light. However, there is even scarcer evidence of magneto-optical effects that can spatially modulate light. Here, we demonstrate the latter by exploiting strongly coupled states of semimagnetic matter and light in planar semiconductor microcavities. We nonresonantly excite two spatially adjacent exciton-polariton condensates which, through inherent ballistic near field coupling mechanism, spontaneously synchronise into a dissipative quantum fluidic supermode of definite parity. Applying a magnetic field along the optical axis, we continuously adjust the light-matter composition of the condensate exciton-polaritons, inducing a supermode switch into a higher order mode of opposite parity. Our findings set the ground towards magnetic spatial modulation of nonlinear light.Comment: 9 pages, 6 figure

    Magnetization dynamics down to zero field in dilute (Cd,Mn)Te quantum wells

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    The evolution of the magnetization in (Cd,Mn)Te quantum wells after a short pulse of magnetic field was determined from the giant Zeeman shift of spectroscopic lines. The dynamics in absence of magnetic field was found to be up to three orders of magnitude faster than that at 1 T. Hyperfine interaction and strain are mainly responsible for the fast decay. The influence of a hole gas is clearly visible: at zero field anisotropic holes stabilize the system of Mn ions, while in a magnetic field of 1 T they are known to speed up the decay by opening an additional relaxation channel
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