Abstract:Here, we report on
the surface conductivity of WSe2 and
MoxW1–xSe2 (0 ≤ x ≤ 1) crystals investigated with conductive atomic
force microscopy. We found that stacking faults, defects, and chemical
heterogeneities form distinct two-dimensional and one-dimensional
conduction paths on the transition metal dichalcogenide surface. In
the case of WSe2, in addition to step edges, we find a
significant amount of stacking faults (formed during the cleaving
process) that strongly influence the surface conductivity. These … Show more
“…As a matter of fact, SBH mapping with nanoscale resolution is required to disentangle the effect of surface (or near surface) defects in the TMD materials from that of metal-induced gap states. To this purpose, the conductive tip of C-AFM has been employed as a nanoscopic metal electrode to record local I-V characteristics on the TMDs surface, from which the SBH was quantitatively evaluated [44,45,69]. Contacting the TMD surface with a sliding metal tip presents the additional advantage of excluding eventual reactions that have been reported at the metal/TMD interface (for some metal species) when the contact is fabricated by evaporation or sputtering [70,71].…”
Section: Schottky Barrier Height Mapping At Metal/tmds Junctionmentioning
confidence: 99%
“…Recently, Bampoulis et al [69] used C-AFM to characterize the conductivity of a Mo x W 1−x Se 2 alloy at the nanoscale. They observed the segregation of Mo-rich and W-rich domains and demonstrated that these different regions exhibit distinct SBHs values, reflecting the different band structures of WSe 2 and MoSe 2 .…”
Section: Lateral Heterojunctions Of Tmdsmentioning
Semiconducting transition metal dichalcogenides (TMDs) are promising materials for future electronic and optoelectronic applications. However, their electronic properties are strongly affected by peculiar nanoscale defects/inhomogeneities (point or complex defects, thickness fluctuations, grain boundaries, etc.), which are intrinsic of these materials or introduced during device fabrication processes. This paper reviews recent applications of conductive atomic force microscopy (C-AFM) to the investigation of nanoscale transport properties in TMDs, discussing the implications of the local phenomena in the overall behavior of TMD-based devices. Nanoscale resolution current spectroscopy and mapping by C-AFM provided information on the Schottky barrier uniformity and shed light on the mechanisms responsible for the Fermi level pinning commonly observed at metal/TMD interfaces. Methods for nanoscale tailoring of the Schottky barrier in MoS2 for the realization of ambipolar transistors are also illustrated. Experiments on local conductivity mapping in monolayer MoS2 grown by chemical vapor deposition (CVD) on SiO2 substrates are discussed, providing a direct evidence of the resistance associated to the grain boundaries (GBs) between MoS2 domains. Finally, C-AFM provided an insight into the current transport phenomena in TMD-based heterostructures, including lateral heterojunctions observed within MoxW1–xSe2 alloys, and vertical heterostructures made by van der Waals stacking of different TMDs (e.g., MoS2/WSe2) or by CVD growth of TMDs on bulk semiconductors.
“…As a matter of fact, SBH mapping with nanoscale resolution is required to disentangle the effect of surface (or near surface) defects in the TMD materials from that of metal-induced gap states. To this purpose, the conductive tip of C-AFM has been employed as a nanoscopic metal electrode to record local I-V characteristics on the TMDs surface, from which the SBH was quantitatively evaluated [44,45,69]. Contacting the TMD surface with a sliding metal tip presents the additional advantage of excluding eventual reactions that have been reported at the metal/TMD interface (for some metal species) when the contact is fabricated by evaporation or sputtering [70,71].…”
Section: Schottky Barrier Height Mapping At Metal/tmds Junctionmentioning
confidence: 99%
“…Recently, Bampoulis et al [69] used C-AFM to characterize the conductivity of a Mo x W 1−x Se 2 alloy at the nanoscale. They observed the segregation of Mo-rich and W-rich domains and demonstrated that these different regions exhibit distinct SBHs values, reflecting the different band structures of WSe 2 and MoSe 2 .…”
Section: Lateral Heterojunctions Of Tmdsmentioning
Semiconducting transition metal dichalcogenides (TMDs) are promising materials for future electronic and optoelectronic applications. However, their electronic properties are strongly affected by peculiar nanoscale defects/inhomogeneities (point or complex defects, thickness fluctuations, grain boundaries, etc.), which are intrinsic of these materials or introduced during device fabrication processes. This paper reviews recent applications of conductive atomic force microscopy (C-AFM) to the investigation of nanoscale transport properties in TMDs, discussing the implications of the local phenomena in the overall behavior of TMD-based devices. Nanoscale resolution current spectroscopy and mapping by C-AFM provided information on the Schottky barrier uniformity and shed light on the mechanisms responsible for the Fermi level pinning commonly observed at metal/TMD interfaces. Methods for nanoscale tailoring of the Schottky barrier in MoS2 for the realization of ambipolar transistors are also illustrated. Experiments on local conductivity mapping in monolayer MoS2 grown by chemical vapor deposition (CVD) on SiO2 substrates are discussed, providing a direct evidence of the resistance associated to the grain boundaries (GBs) between MoS2 domains. Finally, C-AFM provided an insight into the current transport phenomena in TMD-based heterostructures, including lateral heterojunctions observed within MoxW1–xSe2 alloys, and vertical heterostructures made by van der Waals stacking of different TMDs (e.g., MoS2/WSe2) or by CVD growth of TMDs on bulk semiconductors.
“…Alloying in 2D transition metal dichalcogenides (TMDs) has allowed bandgap engineering and phase transformation, which enables a new series of electronic and photonic devices. Bandgap engineering has been demonstrated in various TMD ternary alloys, including MoS 2(1−x) Se 2x , [1][2][3][4][5][6] WS 2(1−x) Se 2x , [7,8] Mo 1−x W x S 2 , [9][10][11][12][13] and Mo 1−x W x Se 2 [14,15] by adjusting the composition of the elements. A 2H-1T' phase transformation was observed in Mo 1−x Re x Se 2 .…”
Device engineering based on the tunable electronic properties of ternary transition metal dichalcogenides has recently gained widespread research interest. In this work, monolayer ternary telluride core/shell structures are synthesized using a one‐step chemical vapor deposition process with rapid cooling. The core region is the tellurium‐rich WSe2−2xTe2x alloy, while the shell is the tellurium‐poor WSe2−2yTe2y alloy. The bandgap of the material is ≈1.45 eV in the core region and ≈1.57 eV in the shell region. The lateral gradient of the bandgap across the monolayer heterostructure allows for the fabrication of heterogeneous transistors and photodetectors. The difference in work function between the core and shell regions leads to a built‐in electric field at the heterojunction. As a result, heterogeneous transistors demonstrate a unidirectional conduction and strong photovoltaic effect. The bandgap gradient and high mobility of the ternary telluride core/shell structures provide a unique material platform for novel electronic and photonic devices.
“…Mechanical exfoliation can consequently induce defect patterns and networks that modify the local electronic structure and chemical reactivity of the basal plane surface. [11][12][13] In principle, the local differences in properties induced by defects can consequently alter the chemical reactivity of the surface. Such heterogeneity can be exploited to produce patterned deposition using defect-selective deposition methods and reaction conditions.…”
Section: D Layered Materials Such As Graphite and Transition Metal mentioning
Atomic layer deposition (ALD) on mechanically exfoliated 2D layered materials spontaneously produces network patterns of metal oxide nanoparticles in triangular and linear deposits on the basal surface. The network patterns formed under a range of ALD conditions, and were independent of the orientation of the substrate in the
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