2018
DOI: 10.1021/acsami.8b10194
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Phase-Engineering-Driven Enhanced Electronic and Optoelectronic Performance of Multilayer In2Se3 Nanosheets

Abstract: Here, we report electronic and optoelectronic performance of multilayer InSe are effectively regulated by phase engineering. The electron mobility is increased to 22.8 cm V s for β-InSe FETs, which is 18 times higher than 1.26 cm V s of α-InSe FETs. The enhanced electronic performance is attributed to larger carrier sheet density and lower contact resistance. Multilayer β-InSe photodetector exhibits an ultrahigh responsivity of 8.8 × 10 A/W under 800 nm illumination, which is 574 times larger than 154.4 A/W of… Show more

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Cited by 56 publications
(64 citation statements)
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References 30 publications
(56 reference statements)
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“…Within them, 2D layered materials have been the most widely studied in recent years owing to the in-plane atoms bonded by strong covalent or ionic bonds and interlayers bonded by weak van der Waals forces, and their smooth surface without chemical dangling bonds, exhibiting excellent electrical, optical and mechanical properties [11][12][13][14]. Ultrathin 2D layered materials are easy to obtain and bandgaps are easy to control benefiting from the unique structure of weak van der Waals forces bonded in interlayers, resulting in great application potential in microelectronics and optoelectronics fields [8,[15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30]. However, 2D non-layered materials with a broad range of properties have rarely been reported in recent years [31][32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…Within them, 2D layered materials have been the most widely studied in recent years owing to the in-plane atoms bonded by strong covalent or ionic bonds and interlayers bonded by weak van der Waals forces, and their smooth surface without chemical dangling bonds, exhibiting excellent electrical, optical and mechanical properties [11][12][13][14]. Ultrathin 2D layered materials are easy to obtain and bandgaps are easy to control benefiting from the unique structure of weak van der Waals forces bonded in interlayers, resulting in great application potential in microelectronics and optoelectronics fields [8,[15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30]. However, 2D non-layered materials with a broad range of properties have rarely been reported in recent years [31][32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…The bandgap can be tuned by adjusting the layer thickness (Figure 2a). [41,44] Another derived phase, β′, was observed to display reversible thermal transit with the β phase with a thickness ranging from 1 layer to ≈20 layers. [43] However, the reason for the stability of 2D β-In 2 Se 3 is unknown.…”
Section: In 2 O 3 In 2 S 3 In 2 Sementioning
confidence: 99%
“…Their potential applications in different fields have been demonstrated. The first class of 2D pS is group III 2 ‐VI 3 ferroelectrics (M 2 X 3 , M = Al, Ga, In; X = S, Se, Te),7,8 and some of them have been synthesized in experiment 4,9–13. Particularly, ferroelectric In 2 Se 3 had been applied to data storage with the switchable polarization, spintronics,9 and visible light absorption 10,14–17.…”
Section: Introductionmentioning
confidence: 99%
“…The first class of 2D pS is group III 2 -VI 3 ferroelectrics (M 2 X 3 , M = Al, Ga, In; X = S, Se, Te), [7,8] and some of them have been synthesized in experiment. [4,[9][10][11][12][13] Particularly, ferroelectric In 2 Se 3 had been applied to data storage with the switchable polarization, spintronics, [9] and visible light absorption. [10,[14][15][16][17] Group III 2 -VI 3 monolayers are also proved to be promising photocatalysts for overall water-splitting with high theoretical solar-to-hydrogen efficiency.…”
mentioning
confidence: 99%