2020
DOI: 10.1021/acsami.0c14201
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Liquid-Phase Exfoliated GeSe Nanoflakes for Photoelectrochemical-Type Photodetectors and Photoelectrochemical Water Splitting

Abstract: Photoelectrochemical (PEC) systems represent powerful tools to convert electromagnetic radiation into chemical fuels and electricity. In this context, two-dimensional (2D) materials are attracting enormous interest as potential advanced photo(electro)catalysts and, recently, 2D group-IVA metal monochalcogenides have been theoretically predicted to be water splitting photocatalysts. In this work, we use density functional theory calculations to theoretically investigate the photocatalytic activity of single-/fe… Show more

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Cited by 67 publications
(73 citation statements)
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“…Consequently, group-IIIA monochalcogenides can be engineered to fulfill the fundamental requirements for the water splitting photo(electro)catalysts, 13 , 21 , 27 i.e., (1) E CBM > reduction energy level of H + /H 2 ( E (H + /H 2 )) and (2) E VBM < reduction energy level of O 2 /H 2 O ( E (O 2 /H 2 O)). 64 66 Despite the existence of few experimental studies on the PEC properties of the most established monochalcogenides, such as InSe, 67 GaSe, 9 and GeSe, 13 no PEC characterizations have been reported for GaS, which is, therefore, a subject matter of interest for the realization of UV-harvesting components in photocatalytic tandem structures (e.g., van der Waals type-I heterojunctions). In this context, the double peak feature around the Γ-point in the so-called “Mexican-hat-like” ring-shaped valence band dispersion of single-/few (≤5)-layer GaS flakes effectively enhances the photoabsorption cross section.…”
Section: Introductionmentioning
confidence: 99%
“…Consequently, group-IIIA monochalcogenides can be engineered to fulfill the fundamental requirements for the water splitting photo(electro)catalysts, 13 , 21 , 27 i.e., (1) E CBM > reduction energy level of H + /H 2 ( E (H + /H 2 )) and (2) E VBM < reduction energy level of O 2 /H 2 O ( E (O 2 /H 2 O)). 64 66 Despite the existence of few experimental studies on the PEC properties of the most established monochalcogenides, such as InSe, 67 GaSe, 9 and GeSe, 13 no PEC characterizations have been reported for GaS, which is, therefore, a subject matter of interest for the realization of UV-harvesting components in photocatalytic tandem structures (e.g., van der Waals type-I heterojunctions). In this context, the double peak feature around the Γ-point in the so-called “Mexican-hat-like” ring-shaped valence band dispersion of single-/few (≤5)-layer GaS flakes effectively enhances the photoabsorption cross section.…”
Section: Introductionmentioning
confidence: 99%
“…Chemically fabricated π-SnS thin film solar cell with the structure of stainless steel (SS)/π-SnS /CdS/ZnO/ZnO:Al/Ag showed η of 1.28% with a relatively higher V OC of 0.470 eV compared to the α-SnS based solar cell [10]. On the other hand, metal monochalcogenides (SiS, SiSe, SiTe, GeS, GeSe, GeTe, SnS, and SnSe) were theoretically predicted to be economical and eco-friendly hydrogen production photocatalysts [12][13][14]. The polymorph of tin sulfide, π-SnS exhibited interesting characteristics such as a high absorption coefficient of 10 −4 cm −1 in the visible region, a direct optical bandgap of 1.7 eV, and a p-type conducting nature with dark conductivity of about 10 −6 Ω −1 cm −1 [9], and had good photoconductivity response [10].…”
Section: Introductionmentioning
confidence: 99%
“…However, the degradation was ascribed to the catalyst detachments, whereas no chemical analysis of CuI after the HER operation was reported. [ 55 ] More recently, 2D materials such as graphene oxide (GO), reduced graphene oxide (RGO), and transition metal dichalcogenides (TMDs) have been demonstrated as efficient CTLs and buffer layers in organic and perovskite solar cells, [ 75–82 ] as well as in other types of photoelectrodes, [ 83,84 ] including those for PEC cells. [ 70,71,85 ] In particular, GO‐ and RGO‐based HTLs and p‐doped MoS 2 have boosted the PEC performances of rr‐P3HT:PCBM photocathodes up to, respectively, J 0vsRHE = 6.01 mA cm −2 , V op = 0.6 V, [ 85 ] and J 0vsRHE = 1.21 mA cm −2 ; V op = 0.56 V. [ 71 ] Among 2D TMDs, WS 2 represents one of the most promising candidates for HTLs, thanks to high hole mobility ( ≈ 50 cm 2 V ‐1 s −1 ) and low effective hole reduced mass ( ≈ 0.46).…”
Section: Introductionmentioning
confidence: 99%