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SnS2 Nanoplates: Synthesis and NO2 Sensing Property

2020-05-13SHANWeiFUZhengqianZHANGFaqiangMAMingshengLIUZhifuLIYongxiang

无机材料学报 2020年4期
关键词:硫化物形貌气体

SHAN Wei, FU Zhengqian, ZHANG Faqiang, MA Mingsheng, LIU Zhifu, LI Yongxiang

SnS2Nanoplates: Synthesis and NO2Sensing Property

SHAN Wei1,2, FU Zhengqian1, ZHANG Faqiang1, MA Mingsheng1, LIU Zhifu1,2, LI Yongxiang1,2

(1. Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China; 2. Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China)

Two-dimensional (2D) metal sulfide materials are ideal for use in gas sensing applications due to their low electronic noise and a large specific surface area, and the research on highly efficient and morphologically controllable methods for preparing two-dimensional metal sulfide materials is necessary. Highly crystalline 2D hexagonal SnS2nanoplates (NPs) with different morphologies were prepared by high temperature chemical bath method. SnS2NPs were characterized by different techniques, and their gas sensing properties were further investigated. The results show that when the molar ratio of oleic acid (OAc) to oleylamine (OAm) is 1 : 1, the shape of typical SnS2NPs is a uniform hexagon, with a diameter of about 150 nm and a thickness of 4-6 nm. The gas sensing test shows typical SnS2NPs are responsive to NO2gas, and the sensing process is reversible and selective. The optimal operating temperature is 130 ℃, and the response and recovery time are 98 and 680 s, respectively.

NO2gas; 2D materials; SnS2; chemical bath synthesis; gas sensing detection

With the development of society, the detection of various gases is becoming more and more important in industrial production and environmental protection[1-2]. At present, semiconductor gas sensors based on oxide gas sensing materials are most widely used due to their high sensitivity, ease of fabrication, simple structure and low cost[3]. For example, WO3, ZnO, and SnO2are used to make ethanol, acetone, and nitrogen dioxide sensors, respectively[4-6]. However, most oxide semiconductor gas sensors tend to exhibit high operating temperatures, poor sensing selectivity and high limits of detection (LODs)[7-9].

In recent years, two-dimensional (2D) transition metal dichalcogenides (TMDs) became a research hotspot in the field of nanomaterials[10-11]. TMDs are promising gas sensing materials due to their planar crystal structure, large surface-to-volume ratio and low electronic noise[12-13], which have not received deserved attention. Perkins,[14]prepared a gas sensor using MoS2single- layer nanosheets obtained by the Scotch tape method. It was found that the gas sensor based on this MoS2single- layer nanosheet had a fast response to triethylamine and acetone. The response time of triethylamine gas is less than 15 s, and this sensor can detect triethylamine gas at concentrations as low as 10–8. Studies by Perkins,[14]have also shown that MoS2-based sensors have better selectivity than carbon nanotube sensors. In particular, this MoS2nanosheet sensor has not strength response to water vapor, which is very important for the practical application of the sensor. Li,[15]found that Metal- Oxide-Semiconductor Field-Effect Transistors (MOSFETs) based on MoS2nanosheets prepared by mechanical stripping can detect NO gas at concentrations as low as 0.8×10–6. The synthesis of TMDs nanoplates (NPs) with controlled size has been of scientific and technological interest. Although tin is not belong to transition metal, SnS2shares the similar layered structure with the TMDs. SnS2has a layered hexagonal structure (=0.3645 nm,=0.5891 nm, space group: P3m1). It is composed of tin atoms sandwiched between two layers of hexagonally disposed close packed sulfur atoms, the adjacent sulfur layers are connected by the weak van der Waals bonding. Bulk SnS2is a semiconductor with a band gap of 2.35 eV[16], which offers interesting applications in the fields of gas sensing. In the past few years, a few preparation methods have been developed for preparing ultrathin SnS2NPs. Huang,[17]reported a FET based on monolayer SnS2flake by exfoliating SnS2crystals and explored its potential application in photodetection. Su,[18]obtained the thin crystal arrays of SnS2at predefined locations, introducing a new idea for large-scale production by chemical vapor deposition. Unfortunately, due to obstacles such as high cost, difficulty of control, small output, the exfoliating and CVD methods are difficult to be used for large-scale production. Therefore, a facile, inexpensive and productive synthesis approach for SnS2NPs with good morphology and reduced thickness is still an important step to explore its future actual application. So simply synthesis route of wet chemistry method have attracted the attention of researchers.

However, the raw materials used in the reported hydrothermal approaches, especially the organometallic precursors and sulphureous sources (carbon disulfide, thioacetamide, thiourea), are toxic and expensive, thus limiting their practical applications[16,19-20]. Recently, Kumar,[21]prepared SnS2hexagonal nanoplates (NPs) by hydrothermal synthesis, with SnCl4·5H2O and sulfur used as precursors, which are cheap and environmental friendly. But the lateral size of these SnS2NPs is less than 60 nm, and the standard diameter of 2D materials is 100 nm[22]. In addition, Du,[23]demonstrated a one-pot chemical solution-phase approach to synthesize SnS2nanoplates using SnCl4·5H2O and sulfur powder as precursors. The size of samples is uniform, but their thickness is (35±10) nm, which may mask some unique properties of few-layer-structure SnS2NPs.

In this work, we report a facile chemical bath method to synthesize uniform 2D SnS2NPs in the presence of oleylamine (OAm), and oleic acid (OAc). The gas sensing results of the typical 2D SnS2NPs show a high response, selectivity, as well as low operating temperatures toward NO2.

1 Experimental

1.1 Reagents

Tin (IV) chloride (SnCl4·5H2O,99.9%, Aladdin) and sulfur powder (99.999%, Aladdin) were used as tin and sulfide precursor, respectively; oleic acid (OAc,90.0%, Aladdin) and oleylamine (OAm,90.0%, Aladdin), were used as surfactant; octadecene (ODe,90.0%, Aladdin) was solvent. All the chemical reagents were used as received without further purification.

1.2 Materials preparation

Fig. 1 is an experimental steps diagram. A simplified Schlenk line was used to protect the reaction from oxygen and moisture, and the whole synthesis process should be under a persistent flow of high-purity N2. In a typical experiment, SnCl4·5H2O (1 mmol) was added to a mixture of OAc (10 mL) and ODe (20 mL) in a 100 mL three-neck flask. The mixed solution was degassed at 130 ℃ for 0.5 h to remove the moisture and the oxygen. Subsequently, the solution was heated to 280 ℃ within 15 min with a vigorous stir (700 r/min). The OAm-S solution (sulfide powder 2 mmol was dispersed into OAm 10 mL) was injected into the reaction system and the reaction was maintained at 280 ℃ for 30 min. After cooling the solution to room temperature naturally, the yellow-green product was collected and separated from the solution by centrifugation. The product was further washed twice by ethanol and cyclohexane (1/1,/) and finally dispersed in cyclohexane. Besides, different morphologies of products were checked by various amount of OAm/OAc while keep other parameters unchanged. The products are stable in air without further protection for further characterizations.

Fig. 1 Diagram of chemical bath synthesis process of 2D SnS2 NPs

1.3 Characterization

The shape and phase of the resulting SnS2NPs were examined by scanning electron microscopy (SEM) JEOL S4800 equipped with an energy-dispersive X-ray spectro­scope (EDS) and transmission electron microscope (TEM) using a JEM-2100F (JEOL) at an accelerating voltage of 200 kV. Powder X-ray diffraction (XRD) patterns were taken on χ’Pert Pro MPD (Philips PANanalytical ) with Cu-Kα radiation at 45 kV and 40 mA. The XRD data was collected with the-2scanning scope started from 2=10º to 80º with a step of 6 (°)/s by using Cu-Kα radiation (0.15418 nm). The composition of the reaction liquid is characterized by Fourier Transform Infrared spectrometer (FT-IR, 8400 Shimadzu, Japan).

1.4 Gas sensing performance test

To make the gas sensing device, 0.1 g of as-prepared typical SnS2NPs and 5 mL of cyclohexane were added into a centrifuge tube with 5 mL capacity. This mixture was ultrasonicated for 10 min to form a concentrated suspension. There are two gold signal electrodes on the front of the flat gas sensing device (shown in Fig. 2(a)) with a platinum wire connecting to each electrode. The SnS2-cyclohexane solution was dropped on the front surface of the device and then dried in ambient air naturally. Repeating the above processes 10 times, a gas sensing tablet whose front surface was completely and evenly covered by SnS2NPs was prepared. On the back of the device there is heating coating of rhodium, and the operating temperature of the gas sensor is controlled by the voltage across the heating coating.

Fig. 2 (a) Schematic diagram of the device for gas sensing testing, and (b) circuit diagram of gas sensing test system

Gas sensing tests were carried out on a self-built measurement system (shown in Fig. 2(b)) using ambient air as the dilute and reference gas. The operating temperature is controlled by the heating voltage applied to the back of the test device. A hygrometer showed a humidity of 60% at room temperature (25 ℃). The sensing time (sen) or recovery time (rec) is expressed as the time for the sensor output reaching 90% of its saturation after the test gas is applied or deactivated in a function step. The responsewas defined as:

whereaandgare the steady-state resistances in air and gas.

2 Results and discussion

2.1 Phase analysis

XRD analysis was applied to identify the crystal structure of typical SnS2NPs. Fig. 3(a) shows the powder XRD pattern of as-prepared SnS2NPs. All the diffraction peaks and relative intensity of samples are in accord with those of bulk SnS2and can be indexed as the 2H hexagonal structure, which is consistent with the standard data file (ICDD 23-0677). The 2H SnS2belongs to the space group (P-3m1) and has three atoms in the unit cell, which extend over only one monolayer. As described in Fig. 3(b), in this SnS2crystal, each Sn atom is six-fold coordinated, hexagonally packed between two three-fold coordinated S atoms, and S-Sn-S quintuple-layers are weakly bonded to other layers by van der Waals force. The primary diffraction peaks of as-prepared SnS2NPs at 2=15.04°, 28.27°, 32.17°, 41.95°, 50.05°, and 52.41° are respectively ascribed to the (001), (100), (101), (102), (110) and (111) planes, which is in accordance with pure 2H SnS2phase.

Fig. 3 (a) XRD pattern of typical SnS2 NPs, and (b) top and cross-sectional schematics of monolayer SnS2

2.2 Morphology analysis

Fig. 4 (a) SEM image of 2D SnS2 NPs, (b) TEM image of 2D SnS2 NPs, (c) cross-sectional HRTEM of 2D SnS2 NPs, (d) zoomed-in HRTEM image, and (e) EDS spectrum of 2D SnS2 NPs

2.3 Reaction principle and morphology control

Here, we discuss the reaction course of SnS2NPs formation in current approach. In the process of heating at 130 ℃, SnCl4·5H2O was dissolved in ODe with the help of oleic acid. It is supposed to be a replacement reaction between SnCl4and oleic acid at high temperature showing in the following reaction equation:

We passed the effluent gas through a flask with deionized water, and after reaction the water became acidic. This proves the formation of hydrochloric acid.

After completion of the reaction, the suspension was allowed to stand for 6 h with 5 mL of ethanol, and the FT-IR spectrum of supernatant is shown in Fig. 5. The presence of strong acyclic C–H stretching at 2924 and 2855 cm–1demonstrates the coexistence of free oleic acid and oleylamine. The discernible peak at 1412 cm–1is assigned to the carboxylate (COO–) stretch, while the obvious peaks at 1560 and 1647 cm–1are attributed to the C–N stretch of amide. Other peaks at 1051, 1083 and 3431 cm–1could be ascribed to vibrations of bonds in ethanol. These FT-IR data confirm that OAm and OAc make amidation reaction and produce H2O, which is consistent with the experimental phenomenon that some low-boiling substances condenses on the upper part of the flask during synthesis reaction. This indicated that when we added the S-OAm solution into the three- necked flask, oleylamine molecules, which had been combined with S, was rapidly amidated with the original oleic acid to form water and rapidly released reactive S.

Fig. 5 FT-IR spectrum of reaction solution

The 2D nano plate morphology arises from the anisotropic bonding nature of SnS2, since the intra-layer covalent bond is stronger than the interlayer van der Waals force. Due to the large amount dangling bonds exist on the edge of the growing nucleation, the growth of SnS2crystals continues with a high anisotropic nature, and Sn and S atoms would selectively bind to these dangling bond sites. Thus, the lateral dimension grows much faster than the vertical thickness dimension, which results in the thin plate morphology of SnS2.

In the typical synthetic method, the molar ratio between oleylamine and oleic acid was about 1 : 1, which resulted in a moderate S generation rate and nucleation rate, and subsequently further reaction prepared typical SnS2NPs with uniform hexagonal shape.

We also investigated the effect of surfactants on the morphology of SnS2NPs. Fig. 6 shows TEM images of SnS2NPs with different molar ratio between OAc and OAm. From Fig. 6(a) to 6(i), the amount of OAm decreases, while that of OAc increases. As shown in Fig. 6(a), with little oleic acid participating in the reaction, the mor­phology of product is quite different from the typical one. Its lateral size is up to 10 μm. When the mixed solution containing S and oil amine was injected into the flask, some of them made amidation reaction with OAc as above and generated SnS2nucleus, while the remai­ning S-OAm solution released H2S[24]. The latter process is much slower than the former, resulting in a low nucleation rate and less number of nucleation. During the whole reaction process, more S and Sn participate in the growth of the NPs; and some of oleylamine molecules tend to interact with S atom exposed on the outer (001) crystal face of SnS2NPs so that the laterial size of this sample is great. As shown in Fig. 6(i), when oleic acid is excessive, almost all OAm moleculars instantaneous amide with OAc moleculars and release a lot of S pre­cursors, which produce much more nucles than those of typical synthe­sis. In addition, excessive OAc mole­culars bonded to Sn atoms exposed on the edge of SnS2NPs, and this interac­tion hinders growing along the lateral dimen­sion. There­fore the morphology of this sample is circle instead of hexagon, and its lateral size is small. The whole reaction and growth process is shown in Fig. 7.

Fig. 6 TEM images of SnS2 NPs with different molar ratio of OAc to OAm from 1 : 9 to 9 : 1 (a-i)

Fig. 7 Growth process of SnS2 NPs

2.4 Gas sensing properties

A large number of studies has demonstrated that the op­erating temperature of a gas sensor is the most infl­uential factor which affects the gas response of semi­conductor sensors[25]. It is known that sulfides are unstable in the air at high temperatures, so we examined the sta­bility of the as-prepared SnS2NPs. After heating the NPs to 150 ℃ in air for 8 d, XRD result showed that there was no tran­sition from SnS2to SnO. And our previous research also shows that SnS2phase tends to fade for the sample treated at 250 ℃[26]. Therefore, we tested the gas sensing response of SnS2NPs at operating temperatures from room temperature to 150 ℃. At room temperature (20 ℃), there is no acceptable signal because the res­istance of the sensing device is too large for the test limit of the ammeter. The response curves of sensors made of typical SnS2NPs in the presence of 10–5of NO2gas at 50–150 ℃ are shown in Fig. 8. The current in the test circuit in the air increased with the growing of tem­perature. This is because more electron- absorbing ther­mal energy transitions from the valence band to the con­duction band, causing the resistance of the material to decrease.SnS2is an n-type semiconductor and NO2molecule is an electron acceptor. When we injected NO2gas into the test chamber, NO2molecules were adsorbed on the surface of SnS2NPs, and electrons in the conduc­tion band of SnS2NPs transferred to NO2molecules, causing the number of conduction band electrons reduc­ing, which made the resistance of SnS2NPs increase[27]. When the temper­ature below 90 ℃, there were less con­duction band electrons. So in NO2atmosphere, almost all elec­trons were transferred to NO2molecules, leading to the fact that resistance was extr­emely large and the cur­rent value was close to 0. At this time,is infinite and the response of SnS2NPs to NO2gas is obvious. At the same time, however, the gas desorption rate at low tem­pera­tures was very slow, and it was clear that when the test device was placed back in the air, the resistance could not return to the pre-adsorption level in an accept­able time range. When the operating tempe­rature reached 130 ℃, the sensing time (sen) and recover time (rec) was 98 s and 680 s, respectively, andwas 4.14. Then, when the temperature continued to rise to 150 ℃,senincr­eased to 168 s andalso decreased to 3.13. So 130 ℃ is the optimum temperature for the detection of NO2gas by SnS2NPs prepared in this study.

Fig. 9(a) shows the dynamic sensing-recovery curves of the sensors to NO2gas with concentrations ranging from 20×10–6to 0.5×10–6at 130 ℃. With the decrease of NO2concentration,was getting weaker and weaker. This is due to less ethanol molecules adsorbed on the surface of the sensing material, and the resistance of SnS2NPs with less change. When the concentration of NO2gas decreased to 0.5×10–6, the gas sensor still per­formed an obvious response, revealing the resistance of the prepared SnS2NPs is very sensitive to NO2gas. Fur­­thermore, we believe that the lowest detection concentra­­tion should be less than 10–7, but due to limitations of experimental conditions, we can’t accurately measure the response signal at lower concentrations.

In order to study their reversibility characteristics, sensing devices were exposed to 10–5of NO2gas and air alternately for 3 or more cycles. In Fig. 9(b), we can see the resistance of sensor in 10–5NO2gas was steady and can return to no-load level after each deso­rption. This result confirms that there is a minuscule amount of gas molecules during desorption process, and this SnS2NPs gas sensors have a good performance in reversible cycle tests. We also tested the responses of this SnS2NPs based sensors to different gases at 130 ℃. Experiments have shown that SnS2NPs was not sensitive to ammonia (100×10–6), carbon dioxide (3%) and hydrogen (20×10–6). This indicates the SnS2NPs based sensors exhibit superior selectivity to NO2gas.

Fig. 8 Response curves of sensors made of typical SnS2 NPs in the presence of 1×10–5 of NO2 gas at different operating temperatures

Fig. 9 (a) Dynamic sensing performance of SnS2 NPs toward NO2 gas at concentrations ranging from 20×10–6 to 0.5×10–6 at 130 ℃, and (b) three reversible test cycles of SnS2 NPs toward 10×10–6 NO2 at 130 ℃

3 Conclusions

Uniform hexagonal shape SnS2NPs with a thickness of 4–6 nm and lateral dimensions of about 150 nm were obtained by high temperature chemical bath method. The ratio between OAm and OAc is the key to control the morphology of SnS2NPs. During the process of nucleus growth, OAm will attach to exposed (0001) crystal surface and prevent NPs vertical growth. To add amount of OAm, we got a series of SnS2nanoplates with huge lateral size. The gas sensing properties of 2D SnS2NPs were investigated at different operating temperatures. 2D SnS2NPs based sensors exhibited excellent sensing properties to NO2gas with a responseof 4.14 at 130 ℃, a sensing time of 98 s and a recovery time of 680 s. This study demonstrates the potential of 2D SnS2NPs for NO2gas sensing applications.

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SnS2纳米片的制备及其对NO2气体的检测

山巍1,2, 傅正钱1, 张发强1, 马名生1, 刘志甫1,2, 李永祥1,2

(1. 中国科学院 上海硅酸盐研究所, 上海 200050; 2. 中国科学院大学 材料与光电研究中心, 北京 100049)

二维金属硫化物材料具有较低的电子噪声以及极大的比表面积, 使其非常适合用作气敏材料, 因此寻求高效可控的方法制备二维金属硫化物材料是目前的研究热点。本研究使用高温化学浴法制备了不同形貌的高结晶二维六方SnS2纳米片。采用不同手段对制备的SnS2纳米片进行表征, 并进一步研究了SnS2纳米片的气敏性能。结果显示: 油酸、油胺用量(体积)相同时, 产物SnS2的形貌是均一的六角形纳米片, 其直径约150 nm, 厚度约4~6 nm。气敏测试表明该SnS2纳米片对NO2气体具有良好响应, 且响应过程可逆, 选择性好。其最佳工作温度为130 ℃, 响应和恢复时间分别为98和680 s。

二氧化氮气体; 二维材料; SnS2; 高温化学浴法; 气敏检测

TQ174

A

2019-3-29;

2019-06-25

National Natural Science Foundation of China (51502325, 61601444)

SHAN Wei(1989–), male, PhD candidate. E-mail: 258897449@qq.com

山巍(1989–), 男, 博士研究生. E-mail: 258897449@qq.com

LI Yongxiang, professor. E-mail: yxli@mail.sic.ac.cn; LIU Zhifu, professor. E-mail: liuzf@mail.sic.ac.cn

李永祥, 研究员. E-mail: yxli@mail.sic.ac.cn; 刘志甫, 研究员. E-mail: liuzf@mail.sic.ac.cn

1000-324X(2020)04-0497-08

10.15541/jim20190133

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