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Hole Conduction of Tungsten Diselenide Crystalline Transistors by Niobium Dopant
Author(s) -
Chu Dongil,
Kim Eun Kyu
Publication year - 2019
Publication title -
advanced electronic materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.25
H-Index - 56
ISSN - 2199-160X
DOI - 10.1002/aelm.201800695
Subject(s) - tungsten diselenide , materials science , doping , dopant , optoelectronics , niobium , transistor , ambipolar diffusion , fermi level , crystalline silicon , characterization (materials science) , nanotechnology , condensed matter physics , silicon , transition metal , electrical engineering , electron , metallurgy , voltage , physics , quantum mechanics , engineering , catalysis , biochemistry , chemistry
Abstract In spite of its ambipolar character, tungsten diselenide (WSe 2 ) is known as one of a few p‐type materials among transition metal dichalcogenides and is currently being used as a fundamental building block of homo‐ and heterojunctions to meet the essential requirement of electronic devices. Many studies have solved the hole transport of WSe 2 by contact engineering; however, another route is shown by an effective p‐doping strategy for achieving reliable p‐type transistor. Diverse characterization methods confirm the transition of the Fermi level from near midgap in intrinsic WSe 2 to lower half bandgap with niobium substitutional doping, leading to a nondegenerate doping level exceeding a 10 17 –10 18 cm −3 hole concentration. As a consequence, current on/off ratio and swing parameter have improved correspondingly as expected. The WSe 2 transistors (with and without doping) are examined by the Zerbst‐type method to conduct the transient data analysis enabling the systemic characterization of the generation lifetime and surface generation velocity of WSe 2 . It is demonstrated that the lifetime for WSe 2 is commonly in the 0.5–0.1 μs range. The generation velocity is ≈10 000‐fold slower than that of the typical crystalline silicon, which is attributed to the ultrathin body nature of the materials.