2015
DOI: 10.1039/c5cc03125g
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Formation of porous SnS nanoplate networks from solution and their application in hybrid solar cells

Abstract: Herein, we present a facile solution-based route towards nanostructured, hybrid absorber layers based on tin mono-sulfide (SnS), an emerging, non-toxic absorber material for low-cost and large-scale PV applications.

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Cited by 43 publications
(34 citation statements)
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“…Since SnS is an indirect bandgap semiconductor, its bandgap is quantificationally evaluated using Kubelka–Munk transformation by plotting ( αhv ) 1/2 versus hv , where α is absorption coefficient, h is Planck constant, and v is photon frequency. As shown in Figure f, bandgap of SnS is extracted to be 1.13 eV, which matches with previous reports …”
Section: Resultssupporting
confidence: 90%
See 1 more Smart Citation
“…Since SnS is an indirect bandgap semiconductor, its bandgap is quantificationally evaluated using Kubelka–Munk transformation by plotting ( αhv ) 1/2 versus hv , where α is absorption coefficient, h is Planck constant, and v is photon frequency. As shown in Figure f, bandgap of SnS is extracted to be 1.13 eV, which matches with previous reports …”
Section: Resultssupporting
confidence: 90%
“…Therefore, it holds great potential to be well integrated into current industrial microelectronics. Second, it manifests rather high absorption coefficient beyond 2 × 10 4 cm −1 across the solar spectrum range, comparable with state‐of‐the‐art photodetecting materials . Third, it is low cost, earth abundant, and nontoxic, establishing solid foundation for its applications …”
Section: Introductionmentioning
confidence: 98%
“…The layered nature of a-SnS has also been attributed to inconsistent growth rates and the uncontrolled formation of SnS lms with needle-, akeor plateletlike morphologies. 4,[11][12][13][14][15][16][17] This poses a signicant challenge for the fabrication of a-SnS thin lm devices, since the morphological implications can result in a high level of grain boundary defects, pin holes, cracks, and an increased interfacial surface area at the p-n junction. All of these features result in higher recombination rates, device shunting or diminished light absorption.…”
Section: Introductionmentioning
confidence: 99%
“…Its large absorption coefficient ($10 5 cm À1 ), 9,10 as well as the predicted high carrier mobility, 7 renders it a great of potential applications in optoelectronic and electronic devices. 2,4,[11][12][13][14][15][16][17][18] Moreover, similar to the black phosphorous (BP) with puckered honey-comb crystal structure, SnS also possesses anisotropic electronic, 19,20 thermoelectric, [21][22][23] piezoelectric 24 and optical 25,26 properties. Given the strongly anisotropic properties of SnS, the SnS-SnS x Se 1Àx core-shell heterostructure with anisotropic photoresponse and the SnS-based photodetector with highly anisotropic performance of near-infrared have been achieved.…”
Section: Introductionmentioning
confidence: 99%