Accepted Manuscript Co3O4 nanoparticles@MOF-5-derived porous carbon composites as anode materials with superior lithium storage performance Yuanyuan Fu, Yanfei Li, Rihui Zhou, Yuzhe Zhang, Shouhui Chen, Yonghai Song, Li Wang PII:
S0925-8388(18)31215-5
DOI:
10.1016/j.jallcom.2018.03.338
Reference:
JALCOM 45568
To appear in:
Journal of Alloys and Compounds
Received Date: 8 January 2018 Revised Date:
18 March 2018
Accepted Date: 27 March 2018
Please cite this article as: Y. Fu, Y. Li, R. Zhou, Y. Zhang, S. Chen, Y. Song, L. Wang, Co3O4 nanoparticles@MOF-5-derived porous carbon composites as anode materials with superior lithium storage performance, Journal of Alloys and Compounds (2018), doi: 10.1016/j.jallcom.2018.03.338. This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.
ACCEPTED MANUSCRIPT
Co3O4 Nanoparticles@MOF-5-Derived Porous Carbon Composites as Anode Materials with Superior Lithium Storage Performance
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Yuanyuan Fu, Yanfei Li, Rihui Zhou, Yuzhe Zhang, Shouhui Chen, Li Wang and Yonghai Song∗ Key Laboratory of Functional Small Organic Molecule, Ministry of Education, Key Laboratory of Chemical Biology, Jiangxi Province, College of Chemistry and Chemical
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Engineering, Jiangxi Normal University, Nanchang 330022, China.
∗Corresponding author: Tel/Fax: +86 791 88120862. E-mail:
[email protected] (Y. Song).
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Co3O4 Nanoparticles@MOF-5-Derived Porous Carbon
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Composites as Anode Materials with Superior Lithium
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Storage Performance
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Yuanyuan Fu, Yanfei Li, Rihui Zhou, Yuzhe Zhang, Shouhui Chen, Yonghai Song and Li Wang∗
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Key Laboratory of Functional Small Organic Molecule, Ministry of Education, Key Laboratory of
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Chemical Biology, Jiangxi Province, College of Chemistry and Chemical Engineering, Jiangxi
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Normal University, Nanchang, 330022, China.
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∗Corresponding author: Tel/Fax: +86 791 88120861. E-mail:
[email protected] (L. Wang). 1
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Abstract A new route to load Co3O4 nanoparticles (NPs) on MOF-5 (MOF-5 was composed of 1,4-
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benzenedicarboxylate (BDC) and Zn2+ via coordination bond (Zn4O(BDC)3•(DMF)8(C6H5Cl)),
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where MOF indicates metal-organic framework) derived hierarchically porous carbon (MDPC) was
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proposed. Various techniques including scanning electron microscopy, transmission electron
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microscopy, Raman spectroscopy, powder X-ray diffraction, X-ray photoelectron spectroscopy,
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thermogravimetric analysis and electrochemical methods were used to characterize the
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Co3O4NPs@MDPC. The results showed that the MDPC contained mesopores obtained by
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vaporizing ZnONPs and micropores came from MOF-5 self. Lots of nano-sized Co3O4NPs formed
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in MDPC’s mesopores. The vast micropores of MDPC provided an effective channel for the
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transport of Li+ when it was used as anode materials for lithium ion batteries (LIBs). The MDPC
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prevented Co3O4NPs from agglomerating effectively, which remained robust for superior rate
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capability during repeated lithiation/delithiation process. And the as-prepared Co3O4NPs@MDPC
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composites remained 94% reversible capacity from the second cycle. Furthermore, the as-prepared
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Co3O4NPs@MDPC anode manifested outstanding capability of 587.2 mA h g-1 at 2000 mA g-1 after
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200 cycles, apparently superior to that of other Co3O4NPs@PC. The high capacity especially at
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high current density and exceptional rate capability of Co3O4NPs@MDPC manifested it is a
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promising anode material for LIBs.
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Keywords: Lithium ion batteries; Porous carbon; Co3O4 nanoparticles; Metal-organic framework
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Introduction Lithium ion batteries (LIBs) are of vital importance in modern life [1,2]. Although graphite is still
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a widely used anode material for LIBs, its low theoretical capacity has not met demands of modern
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life [3,4]. Accordingly, various metal oxide nanomaterials have been proposed for LIBs’ anodes [5-
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9]. Among various metal oxide nanomaterials, Co3O4 nanomaterial is one of the most promising
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anode materials owing to its high theoretical capacity and low cost [10,11]. However, their structure
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destruction due to the huge expansion of volume in the lithation/delithation process would cause the
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increase of irreversible capacity. Furthermore, the poor electron transfer and Li+ diffusion also
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hindered Co3O4 nanomaterials as LIBs’ anode materials.
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To overcome these limitations, one approach is to load Co3O4 nanomaterials on carbon materials
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including graphene [4,12,13], carbon nanotubes [14-16], porous carbon [17,18], etc. These carbon
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materials could enhance electron transfer of Co3O4 nanomaterials. Their good mechanical properties
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could also alleviate structure collapse partly. Among these carbon materials, the porous carbon (PC)
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derived from bio-waste materials has attracted special attention because of its bountiful supply,
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natural hierarchical pores and low cost [19-21]. Some good works have been performed by loading
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Co3O4 nanomaterials on the PC derived from bio-waste materials such as crawfish shell-derived N-
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doped PC [22], animal bones-derived PC networks [23], watermelon-derived carbonaceous
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hydrogel [24], etc. However, the biological sources have inhomogeneous internal structures in the
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different regions, which may result in poor reproducibility. Co3O4 nanomaterials are only loaded on
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the outer surface of PC, which still makes the structure of Co3O4 nanomaterials easy to collapse
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manufacture if the bio-waste materials are unable to access instantly. Another method is to prepare
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Co3O4 nanomaterials@PC by calcining Co-metal organic framework (MOF) [25-29]. However,
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only a few Co3O4 and a large number of Co were formed through calcining Co-MOF. It also is
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difficult to form uniform Co3O4 nanomaterials through calcining Co-MOF owing to Co3O4
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aggregating at high temperature [30,31].
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Hence, a new route to load Co3O4 nanoparticles (NPs) on MDPC (MOF-5 was composed of 1,4-
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benzenedicarboxylate (BDC) and Zn2+ via coordination bond, Zn4O(BDC)3•(DMF)8(C6H5Cl))-
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derived PC) was developed. Herein, lots of nano-sized Co3O4NPs were formed in the mesopores of
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MDPC which was formed by vaporizing ZnONPs. The vast micropores of MDPC originated from
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the MOF-5 increased the specific surface area and facilitated the transport of Li+. The MDPC
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prevented Co3O4NPs from agglomerating, which remained robust for superior rate capability during
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repeated lithiation/delithiation process.
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2. Experimental
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2.1. Reagents and chemicals
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Zn(NO3)2·6H2O and BDC were obtained from Aladdin Industrial Corporation (Shanghai, China).
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Co(CH3COO)2·4H2O was obtained from Sigma-Aldrich and ammonia (25−28 wt%) was purchased
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from Tianjin Yongda Chemical Reagent Factory (Tianjin, China). Dimethyl formamide (DMF) as
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well as ethanol served as solvent were obtained from Guangdong Xilong Chemical Reagent Factory
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(Guangzhou, China). All chemical reagents were used without further purification. Polyvinylidene 4
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Factory (Guangzhou, China). Metallic Li foil (0.6 mm thickness, 99.9%) was purchased from
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Tianjin Zhongneng (Tianjin, China) and copper foil (10 µm thickness) came from Guangzhou
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Jiayuan Company (Guangzhou, China). Millipore-Q System (18.2 MΩ cm) was used to purify tap
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water into ultra-pure water.
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2.2. Preparation of MDPC.
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MOF-5 was prepared via a typical method. Briefly, 1.00 g of BDC and 5.45 g of Zn (NO3)2·6H2O
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were ultrasonic dissolved in 150 mL of DMF. And then, the obtained homogeneous solution was
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transferred into a 250 mL of round flask and subsequently heated to 120 ºC for 4 h in oil bath. Next,
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the raw product was washed with DMF for several times to remove adherent impurity. After dried at
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60 ºC in vacuum oven, pure MOF-5 cube was obtained. As a sacrificial template, the as-mentioned
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MOF-5 was carbonized at 1000 ºC for 3 h at N2 flowing with a heating rate of 5 ºC min-1. Finally,
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the MDPC cube was successfully prepared. The detailed preparation process was diagrammatized
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in Fig. 1.
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2.3. Preparation of Co3O4NPs@MDPC composites
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In a typical procedure, 50 mg of the as-prepared MDPC was dispersed into 96 mL of ethanol and
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then was treated under ultrasonic process for 30 min. Subsequently, 4.4 mL of ultrapure water, 0.36
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g of Co(CH3COO)2·4H2O and 2 mL of 28% ammonia was added into the turbidity solution under
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stirring, respectively. Subsequently, the mixture was stirred in oil bath at 80 ºC for 20 h. And then,
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the solution was sealed in a 100 mL Teflon-lined autoclave, and hold at 150 ºC for 3.5 h. The black 5
ACCEPTED MANUSCRIPT precipitate, Co3O4NPs@MDPC composites, was collected via centrifugation-rinsing cycles and
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dried at 60 ºC overnight. A control sample was prepared in a similar condition by the addition of
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100 mg MDPC (denoted as Co3O4NPs@MDPC-100). The detailed preparation process was
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diagrammatized in Fig. 1. "Here Fig. 1"
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2.4. Characterization
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Scanning electron microscopy (SEM) images were obtained on a HITACHI S3400 performed at
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an acceleration voltage of 20 kV with an Energy dispersive X-ray analyzer (EDXA). Powder X-ray
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diffraction (XRD) analysis was carried out on a D/Max 2500 V/PC X-ray powder diffractometer
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using Cu Kα radiation. X-ray photoelectron spectroscopy (XPS) analysis was obtained by an
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ESCALAB 250Xi spectrometer (ThermoFisher Scientific Co., United States). Thermogravimetric
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analysis (TGA) was acquired on SDT 2960 accompanied with a ramping rate about 10 ºC min-1.
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After exhausting the samples at 200 ºC, N2 adsorption/desorption isotherm was analyzed at liquid
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nitrogen temperature (Tristar 3000) and used to calculate the Brunauer−Emmett−Teller (BET)
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specific surface areas. Transmission electron microscopy (TEM) images were obtained by JEOL
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JEM-2100 microscopes with an acceleration voltage of 200 kV.
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2.5. Electrochemical measurements
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The working electrode was derived from homogeneous slurry which includes active materials,
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acetylene black and PVDF with a weight ratio of 8:1:1. The mixture were added into N-methyl
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pyrrolidinone, and then dispersed evenly on copper foil. Next, the working electrodes were kept at 6
ACCEPTED MANUSCRIPT 60 ºC in a vacuum oven overnight. The thickness of loading active material was 50 µm. The target
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material loaded on copper foil was about 1.0 mg cm-2 and the total weight of active materials in the
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works electrode was about 0.96 mg. The separator is a Celgard 2300 microporous polypropylene
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film. The half-cell was assembled in an argon-filled glove box. The electrolyte was composed of 1.0
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M LiPF6 added in a solvent mixed with ethylene carbonate, diethyl carbonate and dimethyl
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carbonate. Finally, galvanostatic charging/discharging test were carried out at voltage range from
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3.0 to 0.01 V versus Li/Li+ on a Neware BTS test system (Shenzhen, China). Cyclic
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voltammograms (CVs) and electrochemical impedance spectroscopy (EIS) were determined by a
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CHI 760E electrochemical workstation which comes from Shanghai CH Instruments. EIS
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was conducted by applying a perturbation voltage of 5 mV and DC open circuit voltage in the
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frequency range of 100 kHz-0.01 Hz at room temperature. And cells were poised at the selected
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potential for longer than 5 min before measurement. A traditional three-electrode system, lithium
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metal acted as the counter and reference electrode and target materials acted as the working
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electrode, was employed in the above electrochemical test.
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3. Results and discussion
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3.1 Characterization of MDPC
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As shown in Fig. 2A, MOF-5 was a cube with a side length of ~30 µm. The high resolution
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image demonstrated that the MOF-5 cube possessed a flat but ravine surface (Inset in Fig. 2A).
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When annealed at 1000 ºC under N2 flowing, Zn was firstly transformed into ZnONPs and then was
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vaporized completely [32]. The as-obtained MDPC inherited the cubic morphology and generated a 7
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of ZnONPs. TEM image (Fig. 2C) showed that MDPC also contained many meso-/micro-pores
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which might come from MOF-5 self. The elements mapping image (Fig. 2D) and EDS analysis of
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MDPC (Fig. 2E) did not display the element of Zn, indicating that the Zn was evaporated
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completely. Raman spectroscopy of MDPC (Fig. 2F) displayed two typical peaks of carbon, which
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confirmed that the organic ligands were converted into carbon. The XRD diffraction peaks of MOF-
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5 disappeared and no obvious peaks was observed in MDPC (Fig. 2G), further confirming the
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successful transformation. N2 adsorption/desorption isotherms (Fig. 2H) showed that the MOF-5
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cube had a specific surface of 732 m2 g-1, total pore volume of 0.33 cm3 g−1 and a mean pore
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diameter of 1.80 nm, which implied that it was a kind of meso-/microporous material. After heat
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treatment, the specific surface area, the total pore volume and the mean pore diameter of MDPC
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were increased to 2550 m2 g-1, 2.22 cm3 g−1 and 3.5 nm, respectively (Fig. 2H). It clearly suggested
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that the removal of Zn from MOF-5 could effectively enlarge both the pore volume and the pore
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size in MDPC. The larger pores might be used to load nanomaterials.
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"Here Fig. 2"
3.2. Characterization of Co3O4NPs@MDPC
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MDPC was used as a host to load Co3O4NPs in its pores. As shown in Fig. 3A, the cubic shape of
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MDPC was still commendably maintained after the growth of Co3O4NPs. The visible pores became
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small and many granular-like Co3O4NPs were anchored on the surface and holes of MDPC. No
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aggregation and clusters were observed. The elements mapping image (Fig. 3D) showed that the 8
ACCEPTED MANUSCRIPT Co3O4NPs were uniformly formed on the surface and holes of MDPC. TEM image of Co3O4
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NPs@MDPC displayed that abundant black grains was encapsulated in carbon framework and were
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2.5-3 nm or so (Fig. 3B). HRTEM image (Fig. 3C) confirmed that the stripe spacing of two
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different adjacent fringes was 0.23 nm and 0.28 nm, which were contributed to the (222) and (220)
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crystal faces of Co3O4 (JCPDS card NO. 43-1003), respectively. The result clearly proved that
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nano-sized Co3O4NPs were successfully formed in the pores and surface of MDPC. SEM image
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(Fig. S1, Supporting Information) of Co3O4NPs@MDPC-100 showed that its shape still maintained
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but many Co3O4NPs were covered on the surface, which might have a negative effect on the cycle
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stability and the rate capability.
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XRD pattern of Co3O4NPs@MDPC (Fig. 3E) displayed three distinct peaks at 36.9°, 45.1° and
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64.9° which were corresponding to the (311), (400) and (440) diffraction planes of cubic Co3O4
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phase, respectively [5,33]. The result indicated that cubic Co3O4NPs were loaded in the pores of
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MDPC. Raman spectra (Fig. 3F) revealed the short-range local structure of Co3O4NPs@MDPC.
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Besides, the D band and G band assigned to the carbon substrate as well as two characteristic peaks
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belonged to Co3O4NPs appeared. The peak at 473 cm-1 was related to the Eg symmetry, whereas the
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peak at 678 cm-1 was ascribed to A1g species which originated from the octahedral sites [34]. N2
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adsorption/desorption isotherm of Co3O4NPs@MDPC exhibited characteristic IV curve with H4
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hysteresis loop (Fig. 3G). After loading of Co3O4NPs, Brunauer-Emmet-Teller surface area, the
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total pore volume and the mean pore diameter of Co3O4NPs@MDPC reduced to 629 m2 g-1, 0.523
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cm3 g−1 and 1.325 nm, respectively. The result clearly indicated that of the Co3O4NPs covered not
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only on the surface but also in the interior of MDPC. The Co3O4NPs@MDPC still had vast meso-
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/micro-pores, which was benefit for the ion diffusion and mass transfer. To give in-depth understanding of chemical composition and valence state of Co3O4NPs
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@MDPC, XPS was performed. The survey XPS spectrum (Fig. 3H) showed that the Co3O4NPs
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@MDPC mainly contained C, O and Co elements. As shown in inset a (Fig. 3H), C1s spectrum of
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Co3O4NPs@MDPC was resolved into three peaks. Two evident ones at 284.7 eV and 285.5 eV
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were ascribed to C-C bond and C-O bond, respectively. Another weak peak at 287.7 eV was related
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to O-C=O group [22,28]. It was noteworthy that some oxygen-containing functional groups formed
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on the surface of amorphous and graphite carbon frames during the carbonization. As shown in
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high-resolution spectrum of O1s (inset b in Fig. 3H), the peaks were unfolded into lattice Co-O
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bond in Co3O4NPs centered at 530.0 eV, adsorbed O on Co3O4NPs surface centered at 531.5 eV and
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oxygen from surface water at 531.6 eV [6,35]. Furthermore, the high-resolution spectrum of Co2p
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(inset c in Fig. 3H) showed two prominent peaks at 780.0 eV and 795.1 eV, assigned to Co2p3/2 and
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Co2p1/2 orbits, respectively. The binding splitting was 15.1 eV which matched well with those in the
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previous literatures [36,37]. Besides, the Co2p3/2 peak could be fitted with two peaks located at
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780.9 eV and 779.8 eV, indicating that the Co3O4NPs@MDPC consisted of tetrahedral Co2+ and
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octahedral Co3+ [36]. The existence of Co3O4NPs could effectively enhance the energy storage on
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the basis of pure PC.
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"Here Fig. 3” 3.3. Application of Co3O4NPs@MDPC as anode materials for LIBs 10
ACCEPTED MANUSCRIPT For exploring the lithium embedded mechanism of Co3O4NPs@MDPC, the first three CVs of
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Co3O4 NPs@MDPC composites were presented in Fig. 4A in the voltage range from 0.01 V to 3 V
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at 0.2 mV s-1. In the first discharge process, the broad peak appeared at 0.68 V was ascribed to the
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irreversible reaction to form solid electrolyte interphase (SEI) film [29]. Besides, the sharp peak
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centered at 0.91 V was mainly attributed to the transformation of Co3O4NPs into metallic cobalt as
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well as the formation of Li2O [38]. Another two distinct peaks located at 1.4 V and 1.9 V was
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resulted from the reduction of oxygen functional groups on the surface [32]. In the subsequent
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cycles, the cathodic peak at 0.91 V was shifted to 0.94 V, which was correspond to conversion of
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Co3O4 into metallic cobalt. In the first anodic scan, one peak was record at around 2.09 V, which
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was due to the oxidation of metallic cobalt back into Co3O4 and the decomposition of Li2O [39,40].
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In addition, the subsequent cycles almost overlapped with each other, revealing good
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electrochemical stability. Fig. 4B displayed the electrochemical charging/discharging profiles of
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Co3O4NPs@MDPC at 100 mA g-1 in the voltage window between 0.01 V and 3.0 V for the 1st, 2nd,
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3rd, 50th and 100th. After 50 cycles, the electrode of Co3O4NPs@MDPC delivered the specific
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charging and discharging capacities of 1014 mA h g-1 and 873 mA h g-1, respectively. The
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coulumbic efficiency still remained as high as 99.1% after 100 cycles. The good capacities and
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coulumbic efficiency just came from the specific construction: many small Co3O4NPs were loaded
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in the pores of MDPC.
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"Here Fig. 4" To gain insights into the long-term cycle performance, Fig. 5A exhibited the cycling ability of 11
ACCEPTED MANUSCRIPT MDPC, Co3O4NPs@MDPC and Co3O4NPs@MDPC-100 at 2000 mA g-1. After 200 cycles at large
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current density, the specific capacity of Co3O4NPs@MDPC still maintained 587.2 mA h g-1, which
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displayed larger capacity and better capacity retention than that of pure MDPC (only 87.8 mA h g-1)
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and that of Co3O4NPs@MDPC-100 (559.5 mA h g-1). It was remarkable that the combination of
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Co3O4NPs with PC could not only improve electrochemical performance and cycling stability of
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Co3O4NPs, but also partially promote the specific capacity of carbon materials [41]. The lithium ion
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storage at a current density of 2000 mA g-1 was of vital importance in practical application. What’s
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more, the good cycling stability might be credited to the embedding of Co3O4NPs into MDPC
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matrix, which provided strain accommodation against structure collapsing during the repeated
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lithium uptake and removal process. And the CoNPs produced in the discharge process can act as a
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catalyst to effectively facilitate reversible transformation of some SEI components, resulting in
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superior lithium ion storage capacity [38,42,43].
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EIS of Co3O4NPs@MDPC, Co3O4NPs@MDPC-100 and MDPC were displayed in Fig. 5B. The
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diameter of the semicircle of Co3O4NPs@MDPC in high frequency region represented the low
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charge transfer resistance between electrolyte and electrode contact interface of Co3O4
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NPs@MDPC, owing to the superior electron transport of carbon framework. The slope line of
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Co3O4NPs@MDPC in low frequency region, which was more inclined to the Z’ axis, implied a
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lower Warburg resistance due to the well diffusion of Li+ in the electrode, resulting in the enhanced
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electrochemical property.
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excellent rate performance, which achieved capacities of 1418.7, 1388.5, 1162.8, 927.1, and 650
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mA h g-1 at various current densities of 100, 200, 500, 1000, and 2000 mA g-1. When the current
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density was back to 100 mA g-1, the specific capacity even increased to 1500.8 mA h g-1, which
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might be due to the synthetic effect between PC matrix and the appropriate amount of Co3O4NPs as
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well as the complete structures of Co3O4NPs. In addition, SEM image of Co3O4NPs@MDPC after
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100 cycles was presented in Fig. S2 (Supporting Information). It was noticeable that the
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morphology still kept well, suggesting that the pores of carbon skeleton could significantly alleviate
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the structural strain during the lithiation/delithiation.
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"Here Fig. 5"
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In order to gain a intimate comparison, the eletrochemical properties of various carbon/cobalt-
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based composites were listed in Table 1. When
comparing with other materials, the Co3O4
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NPs@MDPC displayed superior specific capacity, cycle life and distinguished rate performance,
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which could be attributed to the porous structure of MDPC matrix, good electrical conductivity and
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uniformly coated lots of nano-sized Co3O4NPs: (1) The pores of MDPC provided high surface for
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loading Co3O4NPs uniformly and buffered the volume variation during the charging/discharging
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process; (2) The MDPC substrate with stable strength prevented Co3O4NPs from aggregating and
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fragmenting; (3) The synergic effect of nano-sized Co3O4NPs and mesoporous structure shortened
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the pathway for Li+ diffusion and charge transfer, thus effectively enhancing the electrochemical
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properties.
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4. Conclusions In a word, the Co3O4NPs@MDPC composites were fabricated by loading nano-sized Co3O4NPs
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(2.5-3.0 nm) on pores of MDPC. The porous cubic nanostructures manifested a long stable cycle
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ability and outstanding discharging/charging specific capacity of 587.2 mA h g-1 at high current
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density of 2000 mA g-1 after 200 cycles, which made it to be a promising material in anode field.
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The enhanced electrochemical performance might be related to the following aspects: (1) The
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supported MDPC matrix alleviated the volume strain during lithium ion insertion/extraction process.
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(2) The porous structure of MDPC provided large specific surface area for loading lots of nano-
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sized Co3O4NPs uniformly and the encapsulated nano-sized Co3O4NPs with stable strength were
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incapable of aggregating and fragmenting; (3) The synergic effect of nano-sized Co3O4NPs and
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mesoporous structure provided a shortened transfer path for lithium ions and electrons, thus
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effectively enhancing the electrochemical properties. The method using the MOF-derived template
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could be applied to prepare other porous composites anode materials for new generation energy
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storage devices.
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Acknowledgements
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This work was financially supported by This work was financially supported by National Natural
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Science Foundation of China (21465014 and 21765009), Science and Technology Support Program
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of Jiangxi Province (20123BBE50104 and 20133BBE50008), Ground Plan of Science and
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Technology Projects of Jiangxi Educational Committee (KJLD14023), and Scientific Research 14
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Foundation of Jiangxi Education Commission (GJJ160288).
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Fig. 1. A schematic representation of the preparation of Co3O4NPs@MDPC composites.
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Fig. 2. SEM images of MOF-5 (A) and MDPC (B). TEM image (C) and corresponding EDX maps
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for C, O, Zn (D) of MDPC. Raman pattern (E) of MDPC, XRD pattern (F) of MOF-5 and MDPC,
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N2 adsorption/desorption isotherm (H) and pore size distribution (inset in H) of MOF-5.
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Fig. 3. SEM images (A), TEM image (B), HRTEM image (C) of Co3O4NPs@MDPC and
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corresponding EDX maps of Co3O4NPs@MDPC for C, O, Co (D). XRD pattern (E), Raman
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pattern (F), N2 adsorption/desorption isotherm (G) and pore size distribution (inset in G), XPS
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spectrum (H) and high-resolution XPS spectrums for C 1s, O 1s and Co 2p (inset in H) of Co3O4
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NPs@MDPC.
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Fig.4. CVs measurements during the first three cycles at 0.2 mV s-1 (A). Galvanostatic
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charging/discharging profiles (B) for the 1st,2nd,3rd ,50th,100th cycles at a current density of 100 mA
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g-1 between 0.01 and 3.00 V of Co3O4NPs@MDPC.
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Fig.5. Cycling performance (A) at 2000 mA g-1 and Rate capability (B) at various current densities
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from 100 mA g-1 to 2000 mA g-1 after three cycles. EIS (C) of Co3O4NPs@MDPC, Co3O4
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NPs/MDPC-100 and MDPC, respectively
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Table 1. Comparison of the electrochemical performance of various carbon and cobalt-based
2
composites as anode materials for LIBs. Current density
Nth
mA g−1
mA h g−1
Mesoporous Co3O4 microcubes
1780
416(60)
[7]
Graphene/Co3O4 Rose-Spheres
90
1110.8 (30)
[12]
Co3O4 @CNT
100
700 (100)
[15]
Porous Hollow Co3O4/N-C
1000
~671 (2000)
[44]
Co3O4/C nanocapsules
445
1026.9 (50)
[45]
Hollow Co3O4/C
50
880 (50)
[46]
890
709 (150)
[47]
890
548(300)
[48]
200
1052(60)
[49]
200
913 (60)
[50]
Porous Hollow Co3O4 Parallelepipeds
100
1100 (50)
[51]
Porous Co3O4 Cuboids
100
886 (60)
[52]
Co3O4 NPs@MDPC
2000
587.2 (200)
This work
References
Mesoporous Co3O4 nanoflake Porous Co3O4 Hollow Tetrahedra
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Highlights
The MDPC matrix possesses a large specific surface area and good electrical conductivity.
The Co3O4NPs loading in MDPC’s pores avoided from agglomerating to endure the volume
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variation. The Co3O4NPs@MDPC exhibited good capability of 578.2 mA h g-1 at 2000 mA g-1 after 200
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The Co3O4NPs@MDPC also exhibited exceptional rate capability.
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cycles.