13,532 research outputs found

    Determining layer number of two dimensional flakes of transition-metal dichalcogenides by the Raman intensity from substrate

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    Transition-metal dichalcogenide (TMD) semiconductors have been widely studied due to their distinctive electronic and optical properties. The property of TMD flakes is a function of its thickness, or layer number (N). How to determine N of ultrathin TMDs materials is of primary importance for fundamental study and practical applications. Raman mode intensity from substrates has been used to identify N of intrinsic and defective multilayer graphenes up to N=100. However, such analysis is not applicable for ultrathin TMD flakes due to the lack of a unified complex refractive index (n~\tilde{n}) from monolayer to bulk TMDs. Here, we discuss the N identification of TMD flakes on the SiO2_2/Si substrate by the intensity ratio between the Si peak from 100-nm (or 89-nm) SiO2_2/Si substrates underneath TMD flakes and that from bare SiO2_2/Si substrates. We assume the real part of n~\tilde{n} of TMD flakes as that of monolayer TMD and treat the imaginary part of n~\tilde{n} as a fitting parameter to fit the experimental intensity ratio. An empirical n~\tilde{n}, namely, n~eff\tilde{n}_{eff}, of ultrathin MoS2_{2}, WS2_{2} and WSe2_{2} flakes from monolayer to multilayer is obtained for typical laser excitations (2.54 eV, 2.34 eV, or 2.09 eV). The fitted n~eff\tilde{n}_{eff} of MoS2_{2} has been used to identify N of MoS2_{2} flakes deposited on 302-nm SiO2_2/Si substrate, which agrees well with that determined from their shear and layer-breathing modes. This technique by measuring Raman intensity from the substrate can be extended to identify N of ultrathin 2D flakes with N-dependent n~\tilde{n} . For the application purpose, the intensity ratio excited by specific laser excitations has been provided for MoS2_{2}, WS2_{2} and WSe2_{2} flakes and multilayer graphene flakes deposited on Si substrates covered by 80-110 nm or 280-310 nm SiO2_2 layer.Comment: 10 pages, 4 figures. Accepted by Nanotechnolog

    Antiferromagnetism and hole pair checkerboard in the vortex state of high Tc superconductors

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    We propose a microscopic state for the vortex phase of BSCO superconductors. Around the vortex core or above H_{c2}, the d wave hole pairs form a checkerboard localized in the commensurate antiferromagnetic background. We discuss this theory in connection with recent STM experiments.Comment: Final versio

    Probing the Electron States and Metal-Insulator Transition Mechanisms in Atomically Thin MoS2 Based on Vertical Heterostructures

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    The metal-insulator transition (MIT) is one of the remarkable electrical transport properties of atomically thin molybdenum disulphide (MoS2). Although the theory of electron-electron interactions has been used in modeling the MIT phenomena in MoS2, the underlying mechanism and detailed MIT process still remain largely unexplored. Here, we demonstrate that the vertical metal-insulator-semiconductor (MIS) heterostructures built from atomically thin MoS2 (monolayers and multilayers) are ideal capacitor structures for probing the electron states in MoS2. The vertical configuration of MIS heterostructures offers the added advantage of eliminating the influence of large impedance at the band tails and allows the observation of fully excited electron states near the surface of MoS2 over a wide excitation frequency (100 Hz-1 MHz) and temperature range (2 K- 300 K). By combining capacitance and transport measurements, we have observed a percolation-type MIT, driven by density inhomogeneities of electron states, in the vertical heterostructures built from monolayer and multilayer MoS2. In addition, the valence band of thin MoS2 layers and their intrinsic properties such as thickness-dependence screening abilities and band gap widths can be easily accessed and precisely determined through the vertical heterostructures
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