2015年5月4日 · Here, we report a reversible structural phase transition between the hexagonal and stable monoclinic (distorted octahedral or 1T′) phases in bulk single-crystalline MoTe 2. Furthermore, an...

2021年2月19日 · The authors used laser-induced phase patterning, a polymorph engineering, to fabricate an ohmic heterophase homojunction between semiconducting hexagonal (2H) and metallic monoclinic (1T') molybdenum ditelluride (MoTe2) that is stable up to 300° and increases the carrier mobility of the MoTe2 transistor by a factor of ∼50, while retaining a ...

2016年5月25日 · Here we detail a reproducible method for chemical vapor deposition of monolayer, single-crystal flakes of 1T′-MoTe 2. Atomic force microscopy, Raman spectroscopy, X-ray photoelectron spectroscopy, and transmission electron microscopy confirm the composition and structure of MoTe 2 flakes.

2019年4月16日 · Here, by combining first-principles calculations and experimental studies, we report on the discovery of robust room-temperature out-of-plane ferroelectricity which is realized in the thinnest...

2018年1月16日 · These distinct quasiparticle scattering behaviors show that 1T'-MoTe 2 is ideal for separating topological and trivial electronic phenomena via temperature-dependent measurements. The Weyl...

2018年4月1日 · Using the polymorphic heteroepitaxy, most recently coplanar semiconductor/metal (2H/1T′) few-layer MoTe 2 heterostructures were experimentally synthesized, highly promising to build circuit components for next generation nanoelectronics.

2016年10月5日 · We study the crystal symmetry of few-layer 1T′ MoTe2 using the polarization dependence of the second harmonic generation (SHG) and Raman scattering. Bulk 1T′ MoTe2 is known to be inversion symmetri...

2025年1月20日 · Mo-based-droplet precursors chemical vapor deposition of monolayer MoTe2 demonstrate slow kinetic growth, showing hexagonal and random ribbon-like morphologies under different temperatures, which als...

2024年10月1日 · In this study, an extraordinary photoluminescence (PL) phenomenon is discovered that originates from a vertical transition between specific bands in the X-point energy valley of K-space in multilayer Weyl semi-metal monoclinic (1T') MoTe2 without a gap structure.

Bulk 1T'-MoTe2 crystals exhibit a max. carrier mobility of 4,000 cm2 V-1 s-1 and a giant magnetoresistance of 16,000% in a magnetic field of 14 T at 1.8 K. In the few-layered form, 1T'-MoTe2 exhibits a bandgap opening of up to 60 meV, which our d. functional theory calcns. identify as arising from strong interband spin-orbit coupling.