Revisiting Intercalation‐Induced Phase Transitions in 2D Group VI Transition Metal Dichalcogenides
Revisiting Intercalation‐Induced Phase Transitions in 2D Group VI Transition Metal Dichalcogenides
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DOI:
10.1002/aesr.202100027
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发表时间:
2021-05
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影响因子:
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通讯作者:
Mengjing Wang;Shiyu Xu;J. Cha
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作者:
Mengjing Wang;Shiyu Xu;J. Cha
2D materials exhibit many exotic structural and electronic phases. Particularly, a 2D-layered transition metal dichalcogenide (TMDC) MX2, with each layer comprising a transition metal layer (M) covalently bonded with top and bottom chalcogen layers (X1⁄4 S, Se, Te), possesses multiple structural polymorphs with distinct physical and chemical properties, as shown in Figure 1A. For example, the trigonal prismatic 2H phase is semiconducting with a thickness-dependent bandgap suitable as a conducting channel in field-effect transistors; the octahedral 1T phase is semimetallic with superior electrochemical catalytic properties; and the distorted octahedral 1T 0/Td phase is topologically protected, exhibiting correlated electronic behaviors, such as the quantum spin Hall effect, spin-resolved Fermi arcs, and even potential topological superconductivity. All the polymorphs (2H, 1T, 1T 0, and Td) can be accessed and transmuted in group VI TMDCs (M1⁄4Mo, W) with transition metals maintaining a d electron configuration, as shown in Figure 1B. It is noted that the thermodynamic stabilities of the phases highly depend on the chalcogen element. For instance, the 2H phase is thermodynamically stable in WS2 at ambient conditions, whereas the Td phase is preferred in WTe2. Such thermodynamic stability distinction can be explained by the energy difference between the 1T/1T 0 and 2H phase, which has a maximum in sulfides and a minimum in tellurides. Typical phase engineering strategies in group VI TMDCs include intercalation of alkali metals, charge doping, strain, high pressure, thermal treatment (heating/cooling), and laser irradiation, most of which accomplish phase conversions by alternating the energetics of the phases. Comprehensive reviews have been written to detail various phase engineering methods. Among the various phase engineering approaches, intercalation of alkali metals into 2D TMDCs has been studied extensively. Intercalation into 2D materials was extensively researched, starting in the 70s. Dresselhaus, Yoffe, and others explored the effects of intercalation on physical properties of 2D materials, such as structural changes, 2D superconductivity, and charge density waves. Despite the extensive investigations and long history in intercalation, microscopic and mechanistic understanding of the intercalation-induced phase transition at the atomic level is just emerging, enabled by the recent developments of multimodal, in situ experimental probes. Because 2D group VI TMDC encompasses an almost complete set of structural polytypes in TMDCs and they are the mostly investigated compounds in the past decade, we will narrow the scope of discussion to group VI TMDCs here. In this Perspective, we will begin by reviewing our current understanding of the phase transition and electrochemical intercalation of alkali metals in group VI TMDCs. Then, we will address gaps in our understanding and suggest critical topics to help build a more complete understanding of the intercalation-induced phase transition in group VI Dr. M. Wang, S. Xu, Prof. J. J. Cha Department of Mechanical Engineering and Materials Science Yale University 15 Prospect St, New Haven, CT 06511, USA E-mail: judy.cha@yale.edu