2016
DOI: 10.1038/nnano.2015.314
|View full text |Cite
|
Sign up to set email alerts
|

Gate-induced superconductivity in atomically thin MoS2 crystals

Abstract: When thinned down to the atomic scale, many layered van der Waals materials exhibit an interesting evolution of their electronic properties, whose main aspects can be accounted for by changes in the single-particle band structure. Phenomena driven by interactions are also observed, but identifying experimentally systematic trends in their thickness dependence is challenging. Here, we explore the evolution of gate-induced The ability to produce few-atom-thick two-dimensional (2D) materials of excellent quality … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...

Citation Types

11
355
0
1

Year Published

2016
2016
2019
2019

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 348 publications
(367 citation statements)
references
References 55 publications
11
355
0
1
Order By: Relevance
“…Additionally, materials with giant spin lifetime anisotropy can provide an exciting platform for manipulating the valley and spin degrees of freedom, and for designing novel spintronic devices. [3,4], where the combined system might be engineered for specific applications [5] or might enable the exploration of new phenomena [6,7]. In the field of spintronics, graphene has exceptional charge transport properties but weak spin-orbit coupling (SOC) on the order of 10 µeV [8], which makes it ideal for long-distance spin transport [9-11] but ineffective for generating or manipulating spin currents.…”
mentioning
confidence: 99%
See 2 more Smart Citations
“…Additionally, materials with giant spin lifetime anisotropy can provide an exciting platform for manipulating the valley and spin degrees of freedom, and for designing novel spintronic devices. [3,4], where the combined system might be engineered for specific applications [5] or might enable the exploration of new phenomena [6,7]. In the field of spintronics, graphene has exceptional charge transport properties but weak spin-orbit coupling (SOC) on the order of 10 µeV [8], which makes it ideal for long-distance spin transport [9-11] but ineffective for generating or manipulating spin currents.…”
mentioning
confidence: 99%
“…Following the discovery of graphene in 2004 [1], a host of other two-dimensional (2D) materials have been synthesized and studied, each demonstrating unique properties and showing promise for technological applications [2]. Currently, there is a great deal of interest in layered heterostructures of these materials [3,4], where the combined system might be engineered for specific applications [5] or might enable the exploration of new phenomena [6,7]. In the field of spintronics, graphene has exceptional charge transport properties but weak spin-orbit coupling (SOC) on the order of 10 µeV [8], which makes it ideal for long-distance spin transport [9][10][11] but ineffective for generating or manipulating spin currents.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, for the trion contribution to the VHE we expect the profile of the measured Hall voltage to be similar to the one shown in Figure 1d: the signal is largest when the laser spot is focused in the center of the Hall probes and decays as the laser beam is scanned away on either side. and MoS 2 , for instance, we have succeeded in observing gate induced superconductivity, 27,28 ambipolar transport of sufficient quality to determine the band gap, 29,30 and in realizing light emitting transistors. 31 The quality of the devices that we have used for the investigation of the VHE is virtually identical to that of the devices used in these past studies, and we refer to the related publications for all general aspects concerning the device electrical characterization.…”
mentioning
confidence: 99%
“…The transistor's electrical properties were characterized by an Agilent B1500A device analyzer in a high vacuum environment (~2×10 -6 Torr) at room temperature (300 K). The transistor shows an ON-OFF ratio (>10 6 ) and a subthreshold swing of ~166 mV/decade (Fig 2a). The clockwise hysteresis loop in the transfer curves originates from interface trapping states [24,25] .…”
mentioning
confidence: 99%