Carbon and few-layer MoS2 nanosheets co-modified TiO2 nanosheets with enhanced electrochemical properties for lithium storage
Tianjin Key Laboratory of Composite and Functional Materials,Tianjin University
Collaborative Innovation Center of Chemical Science and Engineering
收稿日期:5 November 2016
基金:financially supported by the National Natural Science Foundation of China(No.51472177);the China-EU Science and Technology Cooperation Project (No.SQ2013ZOA100006);
Carbon and few-layer MoS2 nanosheets co-modified TiO2 nanosheets with enhanced electrochemical properties for lithium storage
Hui-Hui Lu Chun-Sheng Shi Nai-Qin Zhao En-Zuo Liu Chun-Nian He Fang He
Tianjin Key Laboratory of Composite and Functional Materials,Tianjin University
Collaborative Innovation Center of Chemical Science and Engineering
Abstract:
Carbon and few-layer MoS2 nanosheets comodified TiO2 nanocomposites(defined as MoS2-C@TiO2)were prepared through a facile one-step pyrolysis reaction technique. In this unique nanostructure, the TiO2 nanosheets with stable structure serve as the backbones, and carbon coating and few-layer MoS2 tightly adhere onto the surface of the TiO2. It needs to be pointed out that the carbon coating improves the overall electronic conductivity and the few-layer MoS2 facilitates the diffusion of lithium ions and offers more active sites for lithium-ion storage. As a result, when evaluated as lithium-ion battery anodes, the MoS2-C@TiO2 nanocomposites exhibit markedly enhanced lithium storage capability compared with pure TiO2. A high specific capacity of 180 mA·h·g-1 has been achieved during the preliminary cycles, and the specific capacity can maintain 160 mA·h·g-1 at a high current density of 1 C(1 C=167 mA·g-1) even after 300 discharge/charge cycles, indicating the great potential of the MoS2-C@TiO2 on energy storage.
Keyword:
Few-layer MoS2 nanosheets; Carbon; Co-modified; TiO2 nanosheets; Lithium-ion battery anodes;
Author: Chun-Sheng Shi,e-mail:csshi@tju.edu.cn;
Received: 5 November 2016
1 Introduction
Rechargeable lithium-ion batteries (LIBs),which possess higher power density and longer cycle life,have been regarded as one of the most promising energy storage devices for electrical vehicles
To overcome above obstacles,fabricating TiO2-based nanocomposites is proved to be a common and efficient way via combining with various conductive additives,such as metals
Molybdenum disulfide (MoS2),typical layered transition metal dichalcogenides (TMDs),has attracted great attention as a promising electrode material due to its high theoretical specific capacity and unique two-dimensional layered structure where hexagonal layers of Mo are stuck in two S layers and held together by strong covalent forces,while the MoS2 lamella is bonded by weak van der Waals interactions
Herein,carbon and few-layer MoS2 nanosheets co-modified F-TiO2 nanosheets (defined as MoS2-C@TiO2) were prepared via a simple and facile one-step pyrolysis reaction technique.The microstructure and electrochemical characteristics of MoS2-C@TiO2 nanocomposites were systematically investigated.F-TiO2 nanosheets provide a stable framework in the nanocomposites which allows the uniform dispersion of C and MoS2 on their surface.Importantly,glucose serves as carbon source to improve the electrical conductivity and protect the TiO2 electrode from the direct contact with electrolyte.Furthermore,glucose also is regarded as binder to help few-layer MoS2 nanosheets grow on the surface of TiO2.Besides,few-layer MoS2 nanosheets facilitate a fast insertion/extraction of lithium ions and offer more active sites to improve the specific capacity.When evaluated as the anode material of lithium-ion batteries,the synthesized MoS2-C@TiO2 nanocomposites exhibit high specific capacity and excellent cyclic performance.
2 Experimental
2.1 Preparation of fluorinated TiO2 nanosheets
F-TiO2 nanosheets were prepared using a hydrothermal method reported by Chen et al.
2.2 Synthesis of MoS2-C@TiO2 nanocomposites
MoS2-C@TiO2 nanocomposites were prepared by using a facile one-step pyrolysis reaction technique.In a typical synthesis process,200 mg as-obtained F-TiO2 nanosheets and 100 mg glucose (C6H12O6) were dispersed uniformly into 200 ml deionized water by ultrasonication.Then,22.1 mg sodium molybdate (Na2MoO4·2H2O) and 22.8 mg thiourea (CN2H4S) were added to the above liquid under magnetic stirring to obtain a homogeneous suspension solution.After removing the water of the suspension by freeze-drying technique,the product was ground into fine composite powder.Finally,the as-obtained composite powder was further subjected to calcination at 800℃under the protection of Ar with a heating rate of 10℃·min-1 to synthesize MoS2-C@TiO2 nanocomposites.For comparison,under the same preparation conditions of MoS2-C@TiO2,MoS2-TiO2 and C-TiO2 were also synthesized by calcining the freeze-dried precursor gel without the addition of C6H12O6 and Na2MoO4·2H2O-CN2H4S,respectively.
2.3 Characterizations
Morphologies of the samples were observed by field emission scanning electron microscope (FESEM,HITACHI S4800) and high-resolution transmission electron microscope (HRTEM,JEOL JEM-2100f).The energy-dispersive X-ray (EDX) mapping was performed along with TEM.X-ray diffraction (XRD) patterns were recorded on an X-ray diffractometer (Bruker,D8 Advanced).Thermogravimetric(TG) analysis was performed with a PerkinElmer (TA Instruments) up to 700℃at a heating rate of 10℃·min-1 in air.X-ray photoelectron spectroscopy (XPS) analyses were carried out on a PHI-5000 Versa Probe.And the BrunauerEmmett-Teller (BET) surface areas were measured by nitrogen adsorption isotherms using an autosorb-iQ instrument (Quantachrome,USA).The pore volume,pore diameter and pore size distribution data were calculated using the Barrett-Joyner-Halenda (BJH) method.
2.4 Electrochemical measurements
The electrochemical tests were performed using two-electrode coin-type cells.The coin cells (CR2032) were assembled in an Ar-filled glove box,where lithium metal was used as cathode,Celgard 2400 polypropylene as separator and LiPF6 (1 mol·L-1) dissolved in ethylene carbonate/dimethyl carbonate/diethyl carbonate (EC/DMC/DEC,volume ratio of 1:1:1) as electrolyte.The working electrode slurry was prepared by mixing the active materials,conductive agent (carbon black) and binder(polyvinylidene fluoride,PVDF) in N-methyl-2-pyrrolidinone (NMP) with a mass ratio of 70:15:15.The homogeneous slurry was spread onto a copper foil and then dried in a vacuum oven at 80℃.Cyclic voltammetry (CV) measurement was taken by using a CHI660E electrochemical workstation in the voltage range of 0.5-3.0 V (vs.Li+/Li)at a scan rate of 0.1 mV·s-1.The galvanostatic discharge and charge measurements (GDC) of the batteries were taken using a battery testing system (LAND CT 2001 A,China) at different current densities between 0.5-3.0 V (vs.Li+/Li) at room temperature.Electrochemical impedance spectroscopy (EIS) was recorded on a Gamry Interface1000 electrochemical workstation in the frequency range from 100 kHz to 100 mHz.All of the specific capacities were calculated on the basis of the total weight of MoS2-C@TiO2,MoS2-TiO2 and F-TiO2.
3 Results and discussion
3.1 Morphology and structure
The fabrication procedure of the MoS2-C@TiO2nanocomposites is schematically depicted in Fig.1.Firstly,the F-TiO2 nanosheets are homogeneously dispersed in the C6H12O6-Na2MoO4-CN2H4S aqueous solution (Fig.1a),where F-TiO2 preferentially adsorbed glucose molecules via F abundantly contained on the surface (Fig.1b).Then,
Figure 2 exhibits XRD patterns,SEM and TEM images of the obtained F-TiO2 and MoS2-C@TiO2 nanocomposites.Figure 2a shows that the diffraction peaks of F-TiO2agree well with the standard XRD pattern of anatase TiO2(JCPDS card No.21-1272).After the reaction,the MoS2-C@TiO2 nanocomposites do not exhibit typically diffraction peaks of C and MoS2,although C and MoS2 have been successfully prepared according to SEM and TEM results.This phenomenon is attributed to the small content of MoS2 and C (seen in subsequent XPS results)
For comparison,the morphologies of the samples C-TiO2 and MoS2-TiO2 are shown in Fig.3.For C-TiO2,the TiO2 nanosheets are entirely covered by carbon according to HRTEM image (Fig.3a).For MoS2-TiO2composite (Fig.3b),the TiO2 is separated from MoS2nanosheets and the obtained MoS2 nanosheets turn to aggregation.Therefore,the above results further confirm that glucose serves as the binder to help those few-layer MoS2 nanosheets grow on its surface and prevent MoS2nanosheets from aggregation.
Fig.1 Schematic illustration of procedure for one-step synthesis of MoS2-C@TiO2:a F-TiO2 nano sheets dispersed in C6H12O6-Na2MoO4-CN2H4S aqueous solution,b absorption of C6H12O6 on surface of F-TiO2 nanosheets,c absorption of Na2MoO4-CN2H4S precursor on surface of F-TiO2@C6H12O6 nanosheets and d few-layer MoS2-C@TiO2 nanocomposites after pyrolysis process
Fig.2 a XRD patterns of F-TiO2 and MoS2-C@TiO2,b SEM images and d TEM image of F-TiO2,c SEM image and e,f TEM images of MoS2-C@TiO2,g STEM image of MoS2-C@TiO2,and EDX mapping images of h C,i Ti,j O,k Mo and I S
In order to estimate the content of every component in the MoS2-C@TiO2 nanocomposites,TG analysis was carried out firstly (Fig.4).According to the literature reported previously
Nitrogen adsorption measurements were taken at 77 K to examine the surface area and pore size of the F-TiO2nanosheets and MoS2-C@TiO2 nanocomposites (Fig.5a),and the results are summarized in Table 1.The pore size distribution was calculated using the Barrett-Joyner-Halenda (BJH) method.F-TiO2 nanosheets exhibit a broad range of pore sizes from 10 to 20 nm,indicating a typical mesoporous structure.After the pyrolysis process,the MoS2-C@TiO2 nanocomposites display two kinds of pore,with average pore size of 2 and 4 nm,respectively(Fig.5b).Based on TEM observation,these mesopores imply that the surface of TiO2 nanosheets is decorated with produced C and MoS2.Besides,the MoS2-C@TiO2nanocomposites exhibit a specific surface area of139.1 m2·g-1,which is higher than that of F-TiO2nanosheets (91.4 m2·g-1).The increased specific surface area suggests more accessible contact with the electrolyte and promotes the transport kinetics of lithium ions in the MoS2-C@TiO2 nanocomposites.
XPS tests were carried out to investigate the chemical characteristics of the surfaces of F-TiO2,C-TiO2 and MoS2-C@TiO2 (Fig.6).The spectra show that F element is only presented in F-TiO2 (Fig.6a),and F in TiO2 would easily be removed by heat treatment
Fig.4 TG analysis profile of MoS2-C@TiO2
3.2 Electrochemical performance
LIBs are the state-of-the-art energy storage devices for electric vehicles and hybrid electric vehicles.TiO2 and its derived nanocomposites have been considered as the promising active materials for lithium-ion battery anodes,on account of their cycle stability and service safety.Therefore,the as-prepared MoS2-C@TiO2 nanocomposites have been performed for LIBs anodes as a proof-of-concept application.The lithium storage mechanism of the MoS2-C@TiO2 nanocomposites was explored by CV curves,as shown in Fig.7a.During the discharge process,there are three cathodic peaks at the initial cycle.The peak located at1.7 V is attributed to the intercalation of Li+into TiO2,resulting in the formation of LixTiO2 (Reaction 1)
Fig.3 TEM images of a C-TiO2 and b MoS2-TiO2
Fig.5 a N2 adsorption-desorption isotherms and b pore size distribution of F-TiO2 and MoS2-C@Ti02 (Vads,volume adsorbed;p/p0,relative pressure;Vp,pore volume;Dp,average pore diameter)
Table 1 Specific surface area and pore parameters of F-Tio2 and MoS2-C@Tio2
Fig.6 a XPS full-spectra of F-TiO2,C-TiO2 and MoS2-C@TiO2;high-resolution XPS spectra of b Mo 3d,c S 2p and d O 1s peak in MoS2-C@TiO2
Fig.7 a CV curves at a scan rate of 0.1 mV·s-1 for the first,second and third cycles of MoS2-C@TiO2 over a voltage window of 0.5-3.0 V;b discharge-charge profiles of MoS2-C@TiO2 at a current density of 1.0C (1.0C=167 mA·g-1);c cycling performance of TiO2,C-TiO2,MoS2-TiO2 and MoS2-C@TiO2 nanocomposites;d rate capability of electrode of MoS2-C@TiO2 nanocomposites;e capacity retention of MoS2-C@TiO2 electrode at current densities of 0.1,0.2 and 0.5 A·g-1 for initial four cycles and then 1 A·g-1 for subsequent 1200 cycles
In the charge process,the unconspicuous anodic peak at1.66 V corresponds to the partial oxidation of Mo,as a result of the small amount of MoS2 in the nanocomposite.Such a phenomenon is in agreement with the previous reports about few-layer MoS2-based anode materials
The cycle behavior of MoS2-C@TiO2 at a current density of 1C is presented in Fig.7c.The MoS2-C@TiO2nanocomposites exhibit a relatively high specific capacity coupled with an excellent cycling stability.Unexpectedly,a relatively high capacity of 292 mA·h·g-1 can be achieved in the first discharge process,while it also delivers an irreversible capacity of 231 mA·h·g-1 after the electrode was fully charged to 3 V at the initial cycle,revealing a high initial Coulombic efficiency (CE) calculated to be80%.The irreversible capacity loss is caused by the decomposition of electrolyte.In spite of the fact that the initial CE is 80%,it rapidly increases to above 95%from the fourth cycle and remains above 99%in the following cycles.Importantly,the MoS2-C@TiO2 still can deliver a high specific capacity of 160 mA·h·g-1 even after 300 fast discharge/charge cycles,with a capacity retention of 89%compared with the stable capacity recorded from the second cycle,which indicates a quite low average capacity fading of 0.04%per cycle.In contrast,the cycle behaviors of TiO2,C-TiO2 and MoS2-TiO2 at a current density of 1C are also displayed.From the profiles,the specific capacity of pure TiO2 nanosheets is about 90 mA·h·g-1 after 300cycles and the specific capacity of C-TiO2 does not show an obvious improvement.The C-TiO2 exhibits an initial discharge and charge capacity of 137 and 100 mA·h·g-1,while the reversible capacity fades to 115 mA·h·g-1 after130 cycles.Besides,the capacity of MoS2-TiO2 composites also demonstrates a significant capacity decrease from 170to 100 mA·h·g-1 after 300 cycles,with a capacity retention of only 58.9%(compared with the initial discharge capacity).It should be attributed to the agglomeration of MoS2 nanosheets during the lithiation/delithiation processes,which could cause the remarkably decline of active sites and destruction of 2D microstructure,finally resulting in the severe electrode pulverization as well as material elimination.
The rate performance of MoS2-C@TiO2 nanocomposites was also measured,as presented in Fig.7d.When the current densities increase from 0.5C to 1.0C,2.0C,5.0C and 10C,the reversible specific capacities of the electrode of MoS2-C@TiO2 are 189,159,140,116 and101 mA·h·g-1,respectively.Additionally,it is noteworthy that when the current density reverts to 1.0C from high rates,the capacity can still deliver a high level of150 mA·h·g-1 and maintains stable in the subsequent 50cycles.The aforementioned experimental data give a proof of the fact that our MoS2-C@TiO2 nanostructures do exhibit an excellent rate capability.
To better elucidate the cycle stability at high current density,the MoS2-C@TiO2 nanocomposites were tested at1 A·g-1as presented in Fig.7e.As can be seen,after the activation process of electrode,the MoS2-C@TiO2nanocomposites exhibit a reversible specific capacity of75 mA·h·g-1 at the 4th cycle.Unexpectedly,the specific capacity is quite stable in the subsequent cycles.Even after1200 deep discharge/charge cycles,a specific capacity of73 mA·h·g-1 still can be achieved,showing a capacity retention of near 100%when compared with the capacity of 75 mA·h·g-1 recorded at the 4th cycle.The above results adequately demonstrate that the MoS2-C@TiO2nanocomposites possess excellent structural stability.
Electrochemical impedance spectrum (EIS) analyses were performed to further investigate the reaction kinetics associated with TiO2 and MoS2-C@TiO2 nanocomposites for lithium storage,as shown in Fig.8a.It is found that the MoS2-C@TiO2 electrode shows a much smaller radius of semicircle in the high-medium-frequency region compared to TiO2 electrode,which suggests that MoS2-C@TiO2nanocomposites possess the faster diffusion efficiency of lithium ions together with the shorter transportation pathways of electrons.Moreover,the relationship curve between the real part of the impedance (Z’) and the inverse square root of angular frequency (ω-1/2) in the low-frequency region describes the mass transfer process in electrode materials,and a low slope of this relationship curve indicates fast Li+diffusion kinetics in the electrode
Fig.8 a EIS curves of F-TiO2 nanosheets and MoS2-C@TiO2 nanocomposites and b linear fits of relationship between Z’andω-1/2 in low-frequency region of F-TiO2 nanosheets and MoS2-C@TiO2 nanocomposites (Z”,Z’andωdenote imaginary part,real part of the impedance and angular frequency,respectively)
According to the above results,it can be deduced that the co-modified synergistic effect and the structural advantages of the MoS2-C@TiO2 nanocomposites are contributed to their excellent electrochemical performance.On the one hand,TiO2 nanosheets provide a stable framework to stabilize the whole nanostructure,while the carbon coating layer improves the electrical conductivity and prevents TiO2 nanosheets from the direct contact with the electrolyte.On the other hand,the few-layer MoS2nanosheets facilitate a fast insertion/extraction of lithium ions and offer more active sites to improve the specific capacity.The enhanced electronic conductivity and ionic conductivity should be originated from the co-modified effect of carbon and few-layer MoS2 nanosheets.As a result,when evaluated as a lithium-ion battery anode,the MoS2-C@TiO2 nanocomposite electrodes exhibit a markedly enhanced lithium storage capability and excellent cycle performance.
4 Conclusion
In summary,a facile one-step pyrolysis reaction method was successfully developed to prepare carbon and fewlayer MoS2 nanosheets co-modified TiO2 nanocomposites,which are considered to be of great benefit to improve both the electronic conductivity and ionic conductivity of TiO2.The as-prepared MoS2-C@TiO2 nanocomposites demonstrate a uniform double-coated structure with high surface areas and uniform mesopores.Importantly,when evaluated as a LIB anode,the nanocomposites exhibit improved specific capacity and cycle stability.A relatively high capacity of 292 mA·h·g-1 can be achieved in the first discharge process,and it also delivers an irreversible capacity of 231 mA·h.g-1 after the electrode was fully charged to 3 V at the initial cycle with a high initial CE of about 80%.The specific capacity decreases slightly from180 to 160 mA·h·g-1 at the current density of 1.0C after300 cycles,revealing a superior cycle stability.The excellent electrochemical properties of MoS2-C@TiO2nanocomposites indicate their great potential in energy storage devices.
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