Abstract:The development of intrinsic vacancies in SnSe single crystals was investigated as a function of annealing temperature by means of positron annihilation spectroscopy accompanied by transport measurements. It has been demonstrated that two types of vacancies are present in single-crystalline SnSe. While Sn vacancies dominate in the low-temperature region, Se vacancies and vacancy clusters govern the high-temperature region. These findings are supported by theoretical calculations enabling direct detection and q… Show more
“…12 Therefore, Se and Te nanoclusters or fewlayer films can occur during crystal growth, especially near the sample edges, as proved in SnSe by positron annihilation spectroscopy. 79 It has also been proved that oxidation at ambient conditions seems to favor the presence of the ARMs. 18,21 On the other hand, it has also been shown that treatment with acid agents, like HCl, HF, and HNO3 lead to formation of Te layers in CdTe, while dilution of bromine in methanol removes the Te layer.…”
Two anomalous broad bands are usually found in the Raman spectrum of bulk and 2D Te-based chalcogenides, which include binary compounds, like ZnTe, CdTe, HgTe, GaTe, GeTe, SnTe, PbTe, GeTe2,...
“…12 Therefore, Se and Te nanoclusters or fewlayer films can occur during crystal growth, especially near the sample edges, as proved in SnSe by positron annihilation spectroscopy. 79 It has also been proved that oxidation at ambient conditions seems to favor the presence of the ARMs. 18,21 On the other hand, it has also been shown that treatment with acid agents, like HCl, HF, and HNO3 lead to formation of Te layers in CdTe, while dilution of bromine in methanol removes the Te layer.…”
Two anomalous broad bands are usually found in the Raman spectrum of bulk and 2D Te-based chalcogenides, which include binary compounds, like ZnTe, CdTe, HgTe, GaTe, GeTe, SnTe, PbTe, GeTe2,...
“…According to the results described earlier, a microcosmic mechanism of heat-induced surface structure transformation from SnSe into SnSe 2 could be inferred. As the Sn vacancy defect is the common defect in SnSe, [6,18,19] the migration of Sn ion will format the Schottky defect and nanosized Sn congeries upon the surface of SnSe. The sticky surface of the SnSe nanosheet is due to the semimolten Sn congeries.…”
2D tin selenide (SnSe) is a promising semiconductive material and its thermal stability is one of the most significant evaluating indicators. However, few works are involved in the temperature‐dependent structure stability of 2D SnSe nanosheets. Herein, local structure transformation of a 2D SnSe nanosheet into SnSe2 under high temperature is characterized by a novel atomic force microscope (AFM)‐based nanoscale thermomechanical method. Based on an AFM platform, the temperature‐dependent nanomechanical properties are investigated. A softness process is found to occur upon the surface of 2D SnSe, accompanying the structure transformation under high temperature. It means that the generation of SnSe2 is due to the structure collapse of SnSe, stemming from the evaporation of Sn atoms under about 90 °C. The transformation mechanism is further verified by a real‐time nanothermomechanical method. A deeper understanding of the thermal stability and thermal decomposition mechanism of 2D SnSe is promoted. The improved in situ nanomechanical method offers a highly sensitive method to probing the nanomechanical properties of 2D materials.
“…Successful thermoelectric generators have been made based on SnSe very recently [64]. The effects of vacancy on the thermoelectric properties have been studied in detail [65][66][67][68]. Applied pressure transforms SnSe into a semimetal [69].…”
Neutron powder diffraction and thermoelectric characterization of SnSe:Kx intermetallic alloys are presented. Nanostructured ingots were prepared by arc-melting elemental tin and selenium along with potassium hydride. Up to x = 0.1 of K can be incorporated into SnSe. Rietveld refinement of the diffractograms locates potassium on the Sn site in the high-temperature Cmcm structure. However, in the low-temperature Pnma structure, K cannot be localized by difference Fourier maps, indicating the incorporation of K in a disordered form in the interlayer space. STEM-EELS indicates the incorporation of K into the SnSe grains. The resistivity upon K-doping at intermediate temperatures decreases by 1–2 orders of magnitude, but at high temperature is higher than the undoped SnSe. The Seebeck coefficient of K-doped SnSe remains p-type and almost temperature independent (400 μV/K for x = 0.1). The ultralow thermal conductivity of undoped SnSe decreases further upon K-doping to below 0.3 W/m K.
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