1.1 Introduction
The successful isolation of graphene from bulk graphite [1] has triggered a new burgeoning research area in atomically thin two-dimensional (2D) materials. Since the last decade, several 2D materials namely â graphene, BN, MoS2, MoSe2, WS2, WSe2, MoTe2, Xene sheets (X = Si, Ge, Sn), phosphorene, bismuthene, and many more, have been fabricated and extensively investigated due to their promising applications in the electronic, valleytronic, spintronic, catalysis, energy, and biosensing areas [2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13]. Some of the notable properties that make 2D materials interesting are: high carrier mobility, superconductivity, mechanical flexibility, exceptional thermal conductivity, large photoluminescence, high optical and UV absorption, quantum spin Hall effect, strong lightâmatter interactions, and observation of highly confined plasmonâpolaritons [2, 14, 15, 16]. Interestingly, these properties can be efficiently harnessed in 2D materials by means of strain engineering, number of atomic layers, adsorption, intercalation, interlayer twist, proximity effects, and gate voltage [17, 18, 19, 20]. Furthermore, several types of 2D materials can be vertically stacked to design van der Waals (vdW) heterostructures, which often enhance the desirable properties of the constituent atomic layers [17, 18, 19, 21]. These heterostructures offer unique ways to tailor their remarkable properties, hence they have promising applications in modern technology. However, control of the doping type, carrier concentration, and stoichiometry remains challenging in most of the known 2D materials and vdW heterostructures [21].
Graphene, a two dimensional monolayer of carbon atoms arranged in a honeycomb lattice, has emerged as the most celebrated 2D material of the last decade. It has been thoroughly investigated and many of its interesting features have been revealed [2]. A single layer graphene exhibits numerous novel features such as ultra-high intrinsic mobility (200,000 cm2/Vâ1sâ1), large electrical conductivity, excellent thermal conductivity (5,000 Wâ1Kâ1), biosensing, and exceptional elastic and mechanical properties with a very large Youngâs modulus (~1.0 TPa) [2, 22, 23]. However, the negligible intrinsic spinâorbit coupling (SOC) and correspondingly small energy bandgap limit many practical applications of pristine graphene in spintronics. In recent years, researchers have succeeded in enhancing the bandgap of graphene by several orders using unconventional methods and substrate proximity effects. The availability of many other 2D crystals allows us to design new graphene-based vdW heterostructures having strong proximity effects. A particular family of such 2D crystals is the semiconducting transition metal dichalcogenides (TMDs)-MX2 (M = Mo, W and X = S, Se, Te) â that shows interesting optoelectronic and valleytronic features, and offer strong proximity effects on grapheneâs electronic bandstructure [24, 25, 26, 27, 28].
Atomically thin MX2 semiconductors (M = W, Mo an...