Qi
Lu
a,
Gregory S.
Hutchings
a,
Yang
Zhou
b,
Huolin L.
Xin
c,
Haimei
Zheng
c and
Feng
Jiao
*a
aDepartment of Chemical and Biomolecular Engineering, University of Delaware, Newark, DE 19716, USA. E-mail: jiao@udel.edu
bDepartment of Physics and Astronomy, University of Delaware, Newark, DE 19716, USA
cMaterial Science Division, Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA 94720, USA
First published on 19th March 2014
One-dimensional (1D) electrode materials have attracted much attention recently because of their potential application in flexible battery technology. Many 1D anode materials based on carbon and metal oxides have been synthesized for flexible batteries, however only limited studies on the cathode side have been conducted. Here, we report the synthesis of high-rate cathode electrodes based on Mg-modified LiMnPO4 nanofibers. The nanofibers are embedded inside a nanostructured conducting carbon matrix to enhance their electronic conductivity and structural integrity while retaining flexibility. As a result, a 50% increase in capacity is obtained, achieving an outstanding performance of 135 mA h g−1 at a C/10 rate (15 mA g−1). This nanostructured Mg-modified LiMnPO4 matrix also exhibited superior rate capability and much better cycleability compared to its LiMnPO4 counterpart. Even at a high charge/discharge rate of 5C (750 mA g−1), 80% of the capacity (107 mA h g−1) is still retained, representing, to the best of our knowledge, the best rate performance for LiMnPO4-based electrodes. More importantly, such a superior rate capability is achieved with an excellent cycleability (no capacity fading for 200 deep cycles).
LiMPO4 (M = Fe and Mn) materials are of great interest as promising cathode materials in lithium-ion batteries due to their low cost and good stability.15–23 However, the rate capability of LiMPO4 is greatly limited by its intrinsically low electrical and ionic conductivities.24–28 For LiFePO4, the obstacles were overcome by reducing the size of LiFePO4 particles to nanoscale and introducing a conductive surface coating such as amorphous carbon. These efforts led to the commercialization of LiFePO4 as a cathode material.29–31 Compared with LiFePO4, LiMnPO4 possesses a higher lithium ion intercalation potential of 4.1 V versus Li/Li+ (3.5 V for LiFePO4), providing about 20% higher energy density than that of LiFePO4.32,33 More importantly, the 4.1 V working potential is compatible with most of the liquid electrolytes that are currently in use, while the working potentials for LiCoPO4 and LiNiPO4 (4.8 V and 5.1 V, respectively) are too high for safe operation. Nevertheless, the electronic conductivity of LiMnPO4 is many orders smaller in magnitude than that of LiFePO4, which is already insulating, making it challenging to achieve high rate performance for LiMnPO4 using methods developed for LiFePO4.34 As an additional challenge, the large volumetric change between LiMnPO4 and delithiated MnPO4 during charge/discharge inhibits a smooth lithium ion transport, which results in both lower capacity and limited rate capability.32,35
In the current work, we report a successful preparation of a nanostructured conducting carbon matrix infiltrated with Mg-modified LiMnPO4 as composite cathode electrodes for lithium-ion battery applications. The homogeneous conducting carbon matrix achieved provides efficient electron transport channels, while the nanoscaled size, extended and continuous network facilitates ionic transportation and eliminates the occurrence of intergranular voids. A schematic diagram to represent the design concept is presented in Fig. 1. By introducing a small amount of Mg substitution, the volume change across the two-phase interface is effectively reduced. A high capacity of 135 mA h g−1 (at C/10 rate), a high capacity retention (80% at 5C), and excellent cycle performance are achieved simultaneously.
![]() | ||
Fig. 1 (a) A schematic diagram and (b) an optical image of the flexible carbon matrix infiltrated with Mg-modified LiMnPO4. |
An electrospinning technique followed by a calcination process in inert atmosphere was developed for material synthesis. The morphology of the obtained LiMg0.05Mn0.95PO4 and LiMnPO4 materials are visible in the microscopic images shown in Fig. 2 and S1.† The as-prepared materials were composed of as-spun fibers (Fig. 2a and S1a†) that were long and continuous, with a uniform diameter of approximately 100 nm. The post-calcination process produced the desired C/LiMg0.05Mn0.95PO4 and C/LiMnPO4 composite material network (Fig. 2b and S1b†), accompanied by a slight shrinkage of diameter of the network ligament (Fig. 2c and S1c†). The inert atmosphere during calcination ensured the formation of a homogeneous carbon matrix, infiltrated by the phosphate materials with intrinsically low electrical conductivity. The carbon layer coating was uniform with approximate thickness of 2–4 nm of which the characteristic images are shown in Fig. 2d and S1d.† This is believed to be able to enhance the conductivity of the composite while being thin enough to not interfere with the transport of lithium ions.30,31
Electron energy loss spectroscopy (EELS) characterizations were performed on both LiMg0.05Mn0.95PO4 and LiMnPO4 materials (Fig. 3). As shown in Fig. 3b, no significant changes in the near edge fine structures of Mn were observed for LiMg0.05Mn0.95PO4 and LiMnPO4 compared with MnO, except for instrumental broadening. This indicates that LiMg0.05Mn0.95PO4 shares a same Mn bonding environment as that in LiMnPO4, and is not significantly deviated from that of Mn2+ octahedra in MnO.34 Energy dispersive spectroscopy (EDS) analysis on LiMg0.05Mn0.95PO4 further indicates a successful doping of Mg is achieved because Mg is uniformly distributed throughout the same region as the other elements, P and Mn (Fig. 4).
![]() | ||
Fig. 3 (a) Scanning transmission electron microscopic EELS (STEM-EELS) mapping of Mn, P, and O in LiMnPO4. (b) Comparison of Mn L2,3 (2p->3d) near-edge fine structures of in LiMg0.05Mn0.95PO4, LiMnPO4 and MnO. The reference spectrum of MnO was obtained from ref. 6. |
The crystalline structures of both LiMg0.05Mn0.95PO4 and LiMnPO4 materials were studies with powder X-ray diffraction (PXRD, Fig. 5). The Mg-doped sample showed a very similar profile to that of the un-doped sample except for a peak shift towards higher diffraction angles, indicating the desired smaller unit cell volume. The (311) peaks shown with higher magnification in the inset of Fig. 5 clearly illustrate this feature. Every peak in both profiles could be indexed into an orthorhombic structure, space group Pnma. No impurity was observed. Refinement of the two PXRD patterns was conducted using the Rietveld approach implemented in the software package PDXL (Rigaku). The experimental and the calculated data agree with each other well. The lattice parameters obtained from the refined pattern are shown in Table 1. It clearly shows that the substitution of a small portion of Mg ions results in a successful reduction of the unit cell volume from 304.02 Å3 for LiMnPO4 to 302.52 Å3 for LiMg0.05Mn0.95PO4, which is due to the smaller size of Mg2+ (0.86 Å) compared to Mn2+ (0.98 Å). Additionally, the Mg2+ size is larger than that of Mn3+ (0.785 Å) in the delithiated phase, and therefore a reduction of volume contraction during lithiation/delithiation is believed to be achieved.37,38
![]() | ||
Fig. 5 PXRD patterns and associated Rietveld refinement of LiMg0.05Mn0.95PO4 and LiMnPO4 materials. Inset: peaks corresponding to (311) with higher magnification. |
Material | a/Å | b/Å | c/Å | V Å−3 |
---|---|---|---|---|
LiMg0.05Mn0.95PO4 | 10.446(3) | 6.1027(19) | 4.7457(18) | 302.52(18) |
LiMnPO4 | 10.4645(17) | 6.1141(10) | 4.7516(9) | 304.02(9) |
The electrochemical performance of both electrode materials was evaluated between 2.5 and 4.5 V vs. Li/Li+ at various C rates (1C = 150 mA h g−1). During the charge cycles, cells were trickle charged at the upper voltage limit until the current rate reached C/20. Fig. 6a shows the typical voltage profiles for both LiMnPO4 and LiMg0.05Mn0.95PO4. While their profiles were similar in shape, the capacity performance was significantly different. At a discharge rate of C/10, LiMnPO4 achieved a capacity of less than 90 mA h g−1. However, with only 5% substitution of Mg, LiMg0.05Mn0.95PO4 achieved a dramatically improved capacity of approximately 135 mA h g−1, which amounts to a greater than 50% enhancement.
As proposed, the increase of capacity of LiMg0.05Mn0.95PO4 can be attributed to the enhanced electrochemical kinetics due to the reduced volume and reduced structural mismatch across the lithium ion extraction/insertion interface. While the slightly higher discharge potential of LiMg0.05Mn0.95PO4 (Fig. 6a) might have suggested an improved polarization, electrochemical impedance spectroscopy (EIS) is a more appropriate technique to explore the dynamics at the interface. As shown in Fig. 6b, EIS plots of the LiMg0.05Mn0.95PO4 and LiMnPO4 cells at open circuit potentials were recorded after 10 cycles at C/10 rate. It is clear that the semicircle of LiMg0.05Mn0.95PO4 cells is significantly smaller than that of LiMnPO4, indicating a much smaller charge transfer resistance which is responsible for the great improvement of the electrochemical kinetics of lithium ion extraction/insertion.
The voltage profiles of LiMg0.05Mn0.95PO4 at various charge/discharge rates between C/10 and 6C are presented in Fig. 6c. The un-doped sample showed very similar profiles except for shorter discharge plateaus. Their accordingly calculated cycle capacities are given in Fig. 7. It is clear that LiMg0.05Mn0.95PO4 cells possessed much higher reversible capacity than that of LiMnPO4 cells at all discharge rates. For LiMg0.05Mn0.95PO4, the initial discharge capacity at C/10 is approximately 141.1 mA h g−1 and it averages about 135 mAg g−1 in the first 10 cycles. For the pure LiMnPO4, the initial value is only 92.1 mA h g−1 and averages about 88 mA h g−1 in the first 10 cycles. Even at a high discharge rate of 5C, a discharge capacity of 107 mA h g−1 is still retained for LiMg0.05Mn0.95PO4; for the pure LiMnPO4, the value is only 71 mA h g−1. The results show a successful achievement of more than 50% capacity increase throughout all charge/discharge rates with only 5% Mg substitution. Benefited by the nanostructured conducting carbon matrix, excellent rate performance and ultra-stable cycle performance were simultaneously achieved with both electrode materials. For a 50 times increase of charge/discharge rate from C/10 to 5C, the capacity retention remains as high as 80%. No capacity fade was observed in a 200 cycle test as shown in Fig. 7. The overall performance represents, to the best of our knowledge, the state-of-the-art for LiMnPO4-based electrodes.
![]() | ||
Fig. 7 The cycle performance of the LiMg0.05Mn0.95PO4 and LiMnPO4 cells at various discharge rates (from C/10 to 5C). |
In summary, the current work presents a successful preparation of nanostructured conducting carbon matrix infiltrated by Mg-modified LiMnPO4 and its electrochemical application as a lithium-ion battery cathode. The results demonstrate that introducing a small amount of Mg substitution was able to reduce the volume and structural mismatch between the interfaces of lithium ion extraction/insertion without changing the bonding environment of Mn. The improved electrochemical kinetics was responsible for the great enhancement of material charge capacity. The nanostructured conducing matrix ensured a high material utilization, excellent structural integrity, and fast electron/ion transport rate for achieving excellent rate and cycle performance. The developed synthetic strategy provides a potential pathway for fabricating high-performance electrodes for future flexible lithium-ion storage applications.
Footnote |
† Electronic supplementary information (ESI) available: SEM of LiMnPO4 precursor, TEM and HRTEM of LiMnPO4, STEM-EELS mappings, SEM and TGA data of LiMg0.05Mn0.95PO4 and LiMnPO4. See DOI: 10.1039/c4ta00654b |
This journal is © The Royal Society of Chemistry 2014 |