# Liquid Phase Synthesis of CoP Nanoparticles with High Electrical Conductivity for Advanced Energy Storage

Authors: Guo-Qun Zhang; Bo Li; Mao-Cheng Liu; Shang-Ke Yuan; Leng-Yuan Niu
Journal: Journal of Nanomaterials
 (2017)

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## Abstract

Transition metal phosphide alloys possess the metalloid characteristics and superior electrical conductivity and are a kind of high electrical conductive pseudocapacitive materials. Herein, high electrical conductive cobalt phosphide alloys are fabricated through a liquid phase process and a nanoparticles structure with high surface area is obtained. The highest specific capacitance of 286 F g−1 is reached at a current density of 0.5 A g−1. 63.4% of the specific capacitance is retained when the current density increased 16 times and 98.5% of the specific capacitance is maintained after 5000 cycles. The AC//CoP asymmetric supercapacitor also shows a high energy density (21.3 Wh kg−1) and excellent stability (97.8% of the specific capacitance is retained after 5000 cycles). The study provides a new strategy for the construction of high-performance energy storage materials by enhancing their intrinsic electrical conductivity.


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## Body

## 1. Introduction

Supercapacitors exhibit high power density, fast charging, and long cycling life; they have potential applications in electronic devices, hybrid electric vehicles, and military devices [1–3]. However, the energy density of supercapacitors (4-5 Wh kg−1 for carbon based supercapacitors) is still lower than batteries (30–60 Wh kg−1) and prevents their practical applications [4, 5]. Therefore, many researchers are focused on improving the energy density of supercapacitors while maintaining their high power density [6–8]. The energy storage of pseudocapacitors is based on the Faraday reactions occurring at the surface of electroactive materials, such as RuO2, MnO2, IrO2, and Co3O4 [9–13], and the energy density is higher than carbon based electric double-layer capacitors. Transition metal oxides provide higher specific capacitance and energy density than carbon materials [14, 15], which have been considered as promising pseudocapacitive materials.Among transition metal oxides, cobalt oxides are widely studied as pseudocapacitive materials due to their high specific capacitance, excellent rate capability, and good cycle stability [16–18]. However, the cobalt oxides still suffer from poor electrical conductivity which limits charge/discharge performance at larger current densities [19, 20]. The general strategy for improving conductivity of cobalt oxides is compositing them with high electrical conductive carbons or graphene. For example, Co3O4-reduced graphene oxide scrolls [21], ordered mesoporous carbon composite films containing cobalt oxide and vanadia [22], nitrogen doping graphene based cobalt oxide [23], multiwalled carbon nanotubes, and cobalt oxide film [24] have been fabricated and exhibited better performance than pure cobalt oxide due to the improved electrical conductivity. Unfortunately, the electrical conductivity improvement of adding carbons is limited and the specific capacitance will be decreased when too much carbon is added (because carbon materials would not contribute pseudocapacitance to the composite materials) [25]. Therefore, it is important to look for a new strategy for improving conductivity of cobalt based pseudocapacitive materials. Interestingly, cobalt phosphides possess the metalloid characteristics and superior electrical conductivity (3.17 S cm−1 compared with 10−4 to 10−2 of Co3O4) [26, 27] and are a promising high electrical conductive electrode material of pseudocapacitors. This is because both of the oxidized and reduced cobalt exist in the cobalt phosphide alloys, rather than only oxidized cobalt in the cobalt oxides. The oxidized cobalt in cobalt phosphides could store charges and provide high capacitance through Faradaic reactions, while the reduced cobalt could provide free electrons and greatly improve electrical conductivity. This means that cobalt phosphides will not only possess high capacitance, but also provide high electrical conductivity and excellent rate capability. This inspires us to study the pseudocapacitive performance of high electrical conductive cobalt phosphide alloys.Because of the high electrical conductivity, cobalt phosphides have been studied as materials of lithium ion batteries [28, 29] and supercapacitors [30]. For example, Wang and coworkers [30] have proved that Co2P is an ideal supercapacitive material with good cycle performance and high specific capacity. The study indicates that cobalt phosphide is a promising high electrical conductivity energy storage material. This inspires us to further design and study the electrochemical properties of cobalt phosphide with other crystal phases.Herein, high electrical conductivity CoP nanoparticles with a triangular-pyramid-like structure are further synthesized through a liquid phase process using cobalt acetylacetonate as cobalt precursor and trioctylphosphine as phosphorus source. They show ideal pseudocapacitive properties; the highest specific capacitance is 286 F g−1 at a current density of 0.5 A g−1. 63.4% of the specific capacitance is retained when the current density increased 16 times and 98.5% of the specific capacitance is maintained after 5000 cycles. The AC//CoP asymmetric supercapacitor was assembled using CoP as the positive electrode and activated carbon as the negative electrode which also shows a high energy density (21.3 Wh kg−1) and an excellent stability (97.8% of the specific capacitance is retained after 5000 cycles). The study manifests that CoP alloys are ideal pseudocapacitive materials and have great potential for high-performance electrochemical energy storage systems.


## 2. Experimental Section

CoP particles were synthesized through a liquid phase reaction. 0.5 g cobalt acetylacetonate (purity 98%, shanghai Macklin Biochemical Co., Ltd.), 5 ml of 1-octadecene (purity 90%, SA Chemical Technology (Shanghai) Co., Ltd.), and 0.3 ml of trioctylphosphine (purity 90%, SA Chemical Technology (Shanghai) Co., Ltd.) were added in a three-necked round-bottomed flask. Then the mixture was stirred at 300°C for 5 h. After cooling to room temperature, the sample was washed with normal hexane several times and dried at 80°C for 12 h in vacuum oven. The structure characterizations, electrochemical evaluations, and the preparation of the CoP electrodes are shown in supporting information.


## 3. Results and Discussions

Cobalt and phosphorus atoms arose from the thermal decomposition of cobalt acetylacetonate and trioctylphosphine during the liquid phase reaction, and then CoP particles are formed through the combination between cobalt and phosphorus atoms. Figure1(a) shows the X-ray diffraction (XRD) pattern of the CoP particles. It is obvious that the pattern of CoP is corresponding to the standard patterns of CoP (PDF, card number 29-0497). The diffraction peaks located at 31.62°, 34.56°, 36.34°, 47.74°, 56.70°, 63.06°, 67.95°, and 77.06° can be indexed as (011), (200), (111), (211), (301), (311), (220), and (222) planes of CoP, respectively. The sharp peaks indicate the high crystallinity that is favorable for the CoP to exhibit a high electrical conductivity and even excellent rate capability. However, the XRD pattern of the sample also shows the presence of Co2(P4O12) (PDF, card number 86-2161) in the sample. The low content of Co2(P4O12) phase may be formed through the oxidation of CoP. X-ray photoelectron spectroscopy (XPS) is used to investigate the chemical bonding states of Co and P in cobalt phosphide. The survey spectrum of CoP (as shown in Figure 1(b)) contains the peaks of Co, P, C, and O elements, where the C element is added as master standard for peak position calibration and the O element is derived from surface adsorption of sample when exposed to the air. Figure 1(c) is the Co 2p spectrum. The peaks at binding energy of 781.3 eV and 797.2 eV can be assigned to the Co 2p3/2 and Co 2p1/2 peaks of oxidized Co2+ [31], while the peaks at 778.9 eV and 794.5 eV are corresponding to the Co 2p3/2 and Co 2p1/2 peaks of reduced Co [32]. Besides, the peaks located at 786.0 eV and 803.1 eV are satellites peaks (denoted as “Sat.”). The results indicate that there are two kinds of cobalt (the oxidized Co2+ and the reduced Co) existing in the CoP. Co2+ will be oxidized to Co3+ during the electrode reaction process, which contributes specific capacitance to the CoP electrode, while the reduced Co will provide free electrons and greatly improve electrical conductivity of CoP. It is suggested that the CoP will not only possess high capacitance, but also provide high electrical conductivity, which will serve as an ideal electrode material for pseudocapacitors.Figure 1
(a) XRD pattern of CoP particles. XPS spectra of the CoP (b) survey spectrum and (c) Co 2p.
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(c)The surface morphology and microstructure are shown in Figure2. It can be seen from the scanning electron microscopy (SEM) image (Figure 2(a)) that the CoP exhibits a loosely packed nanoparticles structure and there are abundant interspaces existing between the nanoparticles. This result can further be shown as transmission electron microscope (TEM) image in Figure 2(b). The CoP nanoparticles show a triangular-pyramid-like structure and the size of triangular-pyramid-like nanoparticles is about 20–30 nm. The small size of the CoP nanoparticles will introduce a larger surface area and provide more active sites for the Faraday reactions during charge/discharge process, which will contribute a high specific capacitance. The TEM image also indicates the existence of the interspaces between triangular-pyramid-like nanoparticles. This will provide convenient transportation channels for electrolyte ions and lead to excellent rate capability. The results indicate that the CoP exhibits an ideal morphology and microstructure to serve as pseudocapacitive materials. The porous structure is further characterized by the nitrogen adsorption/desorption experiment (the nitrogen adsorption/desorption isotherms and pore size distribution of CoP are shown in Figure S1 in Supplementary Material available online at https://doi.org/10.1155/2017/9728591). The results indicate that the CoP nanoparticles show a high surface area of 35.4 m2 g−1. It is necessary to possess a large electrode specific surface area for improving the specific capacitances.Figure 2
(a) SEM image and (b) TEM image of CoP particles.
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(b)Figure3(a) shows the CV curves of CoP nanoparticles electrode. The weak redox peaks are observed in each curve, suggesting that the capacitance of CoP electrode is mainly based on the redox mechanism. It is obvious that the shapes of CV curves are close to quasi-rectangular and their enclosed areas are almost distributed in the whole potential window. This means that the surface Faraday reactions of CoP can occur at the whole potential window, suggesting its ideal pseudocapacitive properties. The shape of the CV curves is not significantly influenced by the increase of the scan rates. This indicates the improved mass transportation and electron conduction in the host materials. The fast mass transportation of electrolyte ions to the surface of the CoP electrode could be ascribed to the abundant interspaces between the nanoparticles which provide convenient diffusion channels for electrolyte ions transportation, while the fast electron conduction in the host materials will be attributed to the high electronic conductivity of the CoP. Both the fast mass transportation of electrolyte ions to the surface of the electrode and fast electron conduction in the host materials are beneficial to improve the rate capability of the CoP electrode. To further understand the rate capability and calculate the specific capacitance of the CoP electrode, charge/discharge measurements were performed at various current densities, as shown in Figure 3(b). The curves have a shape like an isosceles triangle that indicates its ideal capacitive behavior. This result is also in accordance with the CV curves. Figure 3(c) exhibits the specific capacitance of the CoP electrode calculated according the discharge curves from the following equation:(1)Cm=I×ΔtΔV×m,whereC is the total capacitance,I is the discharge current, Δt is the discharge time, ΔV represents the potential window,Cm is the specific capacitance, andm is the mass of active materials. The specific capacitance of the CoP electrode is 286 F g−1 at a discharge current density of 0.5 A g−1 and remains 175 F g−1 when the current density is increased to 8 A g−1. Though the specific capacitances gradually decreased at higher current density due to the incremental (IR) voltage drop and insufficient active materials being involved in the redox reaction at higher current, 63.4% of the specific capacitance is still retained when the current density increased 16 times that shows excellent rate capability. This is attributed to the fast mass transportation of electrolyte ions to the surface of the CoP electrode and the fast electron conduction in the host materials of CoP. The cycling stability of the CoP nanoparticles electrode is demonstrated in Figure 3(d). The specific capacitance for the first cycle is 224 F g−1 and then gradually increased in the later cycles due to the fully electrochemical activation of the CoP electrode. Interestingly, the specific capacitance of CoP electrode reached the highest value of 272.2 F g−1 at 2000 cycles and no visible decrease of specific capacitance was found after 5000 cycles. Besides, the coulomb efficiency of the CoP electrode reached 98.5% during 5000 cycles and indicated excellent reversibility of the CoP. Combined with the high specific capacitance, excellent stability, and rate capability, the as-prepared CoP is an ideal material for pseudocapacitors.Figure 3
Pseudocapacitive properties of CoP electrode. (a) CV curves at different scan rates, (b) charge/discharge curves at various current densities, (c) specific capacitance at different current densities, and (d) cycling stability at 2 A g−1.
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(d)For further evaluation of the properties of the CoP electrode, an AC//CoP asymmetric supercapacitor was assembled with CoP as the positive electrode and activated carbon (AC) as the negative electrode. The capacitive performance of AC electrode is shown in Figure S2. It is obvious that the AC electrode exhibits excellent electric double-layer capacitive properties. The specific capacitance reached 206 F g−1 at a discharge current density of 0.5 A g−1. Combined with the specific capacitance and potential window of the CoP electrode, the mass ratio between CoP and AC is calculated according to(2)m+m-=C-m×ΔV-C+m×ΔV+,where C-m and C+m are the specific capacitance of the AC and CoP electrode, ΔV is potential window, andm is the mass of active materials. The calculated mass ratio of CoP/AC is 1 : 1.3. An appropriate voltage window is very important to AC//CoP asymmetric supercapacitor; otherwise there is a risk of damaging the cell when charging it in the high potential. It is considered that the appropriate operation voltage window of AC//CoP asymmetric supercapacitor is 0–1.6 V (Figure S3).The electrochemical test of the AC//CoP capacitor indicates its excellent properties. It shows quasi-rectangular CV curves (Figure4(a)) in the whole voltage range with weak redox peaks, suggesting its ideal pseudocapacitive properties. The shapes of the CV curves remain the same with the increase of the sweep rate, indicating the fast charge/discharge property that is desirable for power devices. The results are also in accordance with charge/discharge curves (as shown in Figure 4(b)) which show a triangle shape. The calculated specific capacitance according to the discharge times is shown in Figure 4(c). It reached 60.3 F g−1 at a discharge current density of 0.5 A g−1 and still retained 44.5 F g−1 at a large discharge current density of 8 A g−1, showing a good rate capability. The excellent cycle stability at a current density of 0.5 A g−1 is also demonstrated in Figure 4(d). The specific capacitance gradually decreased with increase of the cycle numbers and finally 97.8% of the specific capacitance is retained after 5000 cycles.Figure 4
The performance AC//CoP asymmetric supercapacitor. (a) CV curves at different scan rates, (b) charge/discharge curves at various current densities, (c) specific capacitance at different current densities, and (d) cycling stability at 4 A g−1.
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(d)Figure5 shows Ragone plots of AC//CoP, AC//AC, and AC//Co9S8 capacitors. The AC//CoP asymmetric supercapacitor shows higher energy density (21.3 Wh kg−1) than AC//AC symmetric supercapacitors (4.9 Wh kg−1), which reveals that the application of the CoP as the positive electrode can improve energy density of the supercapacitor. What is more, the AC//CoP asymmetric supercapacitor also shows higher energy density than AC//Co9S8 asymmetric supercapacitors (15.1 Wh kg−1) [33], indicating the excellent pseudocapacitive performance and application potentials of the prepared high electrical conductive CoP. The results indicate that the as-prepared high electrical conductive CoP is an ideal pseudocapacitive material.Figure 5
Ragone plots of AC//CoP, AC//AC, and AC//Co9S8 capacitors.


## 4. Conclusion

In summary, high electrical conductive CoP alloys are fabricated through a liquid phase process and a nanoparticles structure with high surface area is obtained. The highest specific capacitance of 286 F g−1 is reached at a current density of 0.5 A g−1. 63.4% of the specific capacitance is retained when the current density increased 16 times and 98.5% of the specific capacitance is maintained after 5000 cycles. The AC//CoP asymmetric supercapacitor also shows a high energy density of 21.3 Wh kg−1 and excellent stability (97.8% of the specific capacitance is retained after 5000 cycles). The study provides a new strategy for the construction of high-performance energy storage materials by enhancing their intrinsic electrical conductivity.



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*Source: 9728591-2017-10-09.xml*