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    Ambipolar MoS<sub>2</sub> Transistors by Nanoscale Tailoring of Schottky Barrier Using Oxygen Plasma Functionalization

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    One of the main challenges to exploit molybdenum disulfide (MoS<sub>2</sub>) potentialities for the next-generation complementary metal oxide semiconductor (CMOS) technology is the realization of p-type or ambipolar field-effect transistors (FETs). Hole transport in MoS<sub>2</sub> FETs is typically hampered by the high Schottky barrier height (SBH) for holes at source/drain contacts, due to the Fermi level pinning close to the conduction band. In this work, we show that the SBH of multilayer MoS<sub>2</sub> surface can be tailored at nanoscale using soft O<sub>2</sub> plasma treatments. The morphological, chemical, and electrical modifications of MoS<sub>2</sub> surface under different plasma conditions were investigated by several microscopic and spectroscopic characterization techniques, including X-ray photoelectron spectroscopy (XPS), atomic force microscopy (AFM), conductive AFM (CAFM), aberration-corrected scanning transmission electron microscopy (STEM), and electron energy loss spectroscopy (EELS). Nanoscale current–voltage mapping by CAFM showed that the SBH maps can be conveniently tuned starting from a narrow SBH distribution (from 0.2 to 0.3 eV) in the case of pristine MoS<sub>2</sub> to a broader distribution (from 0.2 to 0.8 eV) after 600 s O<sub>2</sub> plasma treatment, which allows both electron and hole injection. This lateral inhomogeneity in the electrical properties was associated with variations of the incorporated oxygen concentration in the MoS<sub>2</sub> multilayer surface, as shown by STEM/EELS analyses and confirmed by ab initio density functional theory (DFT) calculations. Back-gated multilayer MoS<sub>2</sub> FETs, fabricated by self-aligned deposition of source/drain contacts in the O<sub>2</sub> plasma functionalized areas, exhibit ambipolar current transport with on/off current ratio <i>I</i><sub>on</sub>/<i>I</i><sub>off</sub> ≈ 10<sup>3</sup> and field-effect mobilities of 11.5 and 7.2 cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup> for electrons and holes, respectively. The electrical behavior of these novel ambipolar devices is discussed in terms of the peculiar current injection mechanisms in the O<sub>2</sub> plasma functionalized MoS<sub>2</sub> surface
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