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Front. Mater., 19 February 2020
Sec. Ceramics and Glass
This article is part of the Research Topic Glasses for Energy Applications View all 9 articles

Crystallization of the Na2FexNi1−xP2O7 Glass and Ability of Cathode for Sodium-Ion Batteries

  • Department of Materials Science and Technology, Nagaoka University of Technology, Nagaoka, Japan

Although the sodium phosphate cathode active materials based on the Ni3+/Ni2+ redox reaction are expected to develop a high discharge potential, none of the studies aimed at practical application have been reported due to its poor kinetics showed in the sodium phosphate. Herein, we substituted active Fe for a part of Ni, expecting to activate the potential deriving from the Ni3+/2+ in Na2FexNi1−xP2O7 glass-ceramics. Precursor glasses were prepared by the melt-quenching method and exhibited surface crystallization tendency due to heterogeneous nucleation. In the charge-discharge testing, all the flat potential showed in the discharge process derived from the reduction of Fe3+/2+. However, from the dQ/dV plot, there were two weak reduction peaks at 4.3 and 4.4 V in the discharge process of Na2Fe0.25Ni0.75P2O7. Combining with the oxidation peak at 4.6 V in the second charge process of Na2NiP2O7, we believe the reduction peaks at 4.3 and 4.4 V were derived from the Ni3+/2+.


At present, Lithium-Ion Rechargeable Batteries (LIBs) are widely applied to small electronic equipment such as mobile phones and laptop computers, due to the high voltage, high energy density, and long charge-discharge cycle life (Nishi, 2001; Nitta et al., 2015). However, high cost and low safety (Spotnitz and Franklin, 2003; Wang et al., 2012; Finegan et al., 2015) are becoming enormous challenges for them. On the other hand, accompanied by the development of science and technology, drastic improvement of the energy and power density is required, so developing new electrode materials is necessary.

Considering the abundance of sodium ions existing (Slater et al., 2013) and the nearest ion radius with lithium-ion in the group of alkali metal elements in the periodic table, quantities of researchers paid their attention to sodium rechargeable batteries. As a matter of fact, due to the dense atomic mass and larger ionic radius, SIBs commonly generate a lower energy density (Kundu et al., 2015) and a shorter cycle life (Ong et al., 2011) than LIBs. Therefore, the object of these problems is the most critical challenge for SIBs. Some researchers focus on cathode materials to promote the storage of sodium ions. There are numerous types of cathode materials for SIBs had been reported, such as transition-metal layered oxides NaxMO2 (Yabuuchi et al., 2012; Wang et al., 2016), Phosphates NaMPO4 (Fang et al., 2015; Bianchini et al., 2018), Pyrophosphates Na2MP2O7 (Honma et al., 2012, 2013; Barpanda et al., 2013b), Fluorophosphates Na2MPO4F (Ellis et al., 2010), Sulfates Na2M2(SO4)3 (Barpanda et al., 2014) and NaM(SO4)2 (Singh et al., 2015). In addition to exploiting the cathode materials, synthesis should be low-cost. Crystallization of glasses is a simple method, which starting from the low-cost precursor glasses for the fabrication of crystalline materials with desired shapes and functions (Komatsu, 2015; Deubener et al., 2018). Glass-forming oxide P2O5 makes this an excellent method to synthesis Phosphates and Pyrophosphates. We have investigated and analyzed the crystallization and electrical performance of some active materials in LIBs or SIBs based on the glass or glass-ceramics (Nagamine et al., 2011, 2012; Honma et al., 2012).

Na2FeP2O7 has been acknowledged that it could be the cathode candidate for the rechargeable sodium-ion second batteries (SIBs). Among the reports about the electrochemical properties of Na2FeP2O7, it exhibited a high potential of 2.9 V and a high discharge capacity of 88 mAh/g, which is 90% of the theoretical capacity based on the glass-ceramics (Honma et al., 2012). Owing to the high thermal stability (Barpanda et al., 2013a) and excellent properties exhibited by the electrochemical charge-discharge testing (Kim et al., 2013), it is looked forward to being used as the positive material in SIBs to instead of LIBs. Besides, Yamauchi demonstrated an oxide all-solid-state battery that positively utilizes the viscous flow of the Na2FeP2O7 precursor glass and a glass-ceramics (Yamauchi et al., 2019). According to the Crystal field splitting of the M2+ cations in octahedral coordination, it indicated that the Ni2+ delivered the highest potential in the lithium or sodium system (Gutierrez et al., 2013). Hence the Ni2+ based on the stable three-dimensional framework composed of (P2O7)4− with Na ions is expected to exhibit a higher potential than that of Fe2+. Unfortunately, Na2NiP2O7 was reported that Ni was not active in the pyrophosphate framework under the electric test (Zhang et al., 2017).

Furthermore, a similar result was also obtained in Na2MnP2O7 glass-ceramics with none activity of Mn2+ (Tanabe et al., 2018). However, in the Na2Fe0.25Mn0.75P2O7 compound with a little Fe substitution, it appeared a high potential of 3.8 V derived from Mn3+/2+ (Tanabe et al., 2018). Therefore, the appearance of Ni3+/2+ in higher potential with Fe substitution is expected. In this study, the crystallization behavior, density, and electrochemical properties of Na2FexNi1−xP2O7 glass or glass-ceramics will be reported for the first time.


The precursor Na2FexNi1−xP2O7 glasses (x = 1, 0.75, 0.5, 0.25, 0) were prepared by melt-quenching method. Under the composition of 33.3Na2O-33.3xFeO-33.3 (1−x) NiO-33.3P2O5 (mol%), the precursor chemicals sodium dihydrogen phosphate (98.0% NaH2PO4, Nakarai Tesque Co., Japan), iron mono-oxide (99.5% FeO, Kojyundo Chemicals Co., Japan) and nickel mono-oxide (99.9% NiO, Kojundo Chemicals Co., Japan) were weighted and mixed. Then the mixed Na2NiP2O7 powder was melted in a platinum crucible at 1,200°C for 30 min in the air atmosphere, and other composition powder was melted in a graphite crucible at 1,200°C for 30 min in the nitrogen atmosphere by an electric furnace. The melt was then poured onto a steel plate and quenched with another steel plate to produce a bulk glass precursor.

In order to confirm the amorphous state and identify the crystalline phase, the X-ray diffraction (XRD) was performed on Rigaku Ultima IV X-ray diffractometer (Rigaku, Japan) equipped with Cu-Ka radiation (40 kV, 40 mA, and λ = 0.154056 nm) in a speed of 5 deg./min between 10 and 70 deg. The density of the samples was determined by using the XS205 Dual Range analytical balance (METTLER TOLEDO, Japan) by the Archimedes principle. Differential thermal analysis (DTA, Thermoplus EVO TG-8120, RIGAKU Corp., Japan) was used to determine the glass transition temperature Tg, glass crystallization onset temperature (Tx), and glass crystallization temperature Tp of the samples. All the processes performed under the N2 atmosphere, and the temperature scanning rate of 10 K min−1. Scanning Electron Microscope (SEM, KEYENECE VE-8800) was used to check the crystallization behavior of the glasses.

Because of the strong covalent bond in the pyrophosphates could lead to a low electric conductivity, so the carbon coating was necessary (Chung et al., 2002). An automatic mortar ground the glass precursors for 30 min and selected by a sieve in which the particle size was under or equaled 105 μm. And then, the mixture composed of glass precursors and carbon black (CB) in a weight ratio of 84.2: 15.8 placed into a ZrO2 pot (45 cm3) together with 50 g balls (3 mm) and 10 ml methanol, so the mixture would be mixed and pulverized for 15 min × 4 cycles in 700 rpm by wet ball-milling (FRITSCH Premium line P7). After wet ball-milling, we used an evaporator (Tokyo Rika Kikai, N-1110V) to distill off the rudimental methanol and dried the mixture (glass/CB) at 80°C for 1 h. In order to fabricate the positive electrode materials, we did a heat-treatment regarding the mixture of Na2FexNi1−xP2O7 glass and CB. Heat-treatment was performed on glass crystallization temperature Tp for 3 h under a nitrogen atmosphere. We used Polyvinylidene fluoride (PVDF) as a binder with the mixture of crystallized Na2FexNi1−xP2O7 glass-ceramics and graphite in a weight ratio 5:95 in a mortar. In order to prepare a slurry to coat on the aluminum foil, we dropped a little N- methylpyrrolidone (NMP) as a solvent to mix with that and dried the coated Al foil at 80°C for 1 h. Finally, the positive electrode was punched out as 16 mmϕ and dried at 100°C in a vacuum oven all night. Sodium metal foils were used as the negative electrodes, the glass filter papers (Advantec Co., GA-100) were used as a separator, and the solution of 1 M NaPF6 in a mixture of ethylene carbonate (EC) and diethyl carbonate (DEC) (1:1, v/v) was used as the electrolyte. The test cells were assembled by the flat cells in an argon-filled glove box, in which the dew point temperature kept at −86°C. The charge-discharge test was performed at a cutoff voltage of 1.5–4.9 V and a rate of 1/10 C by a battery testing system (Hokuto-denko Co.).

The theoretical capacity and corresponding electrochemical reaction formula is showing below:

Theoretical capacity (mAh/g)=          n (mol)×F (C/mol)M (g/mol) ×3600 (s/h) ×1000 (mA/A)

n is the theoretical mole number of the de-insertion sodium ions; F is the Faraday constant; M is the mole mass of the cathode material.

The electrical resistance of glass-ceramics was measured in the form of a pellet with a thickness of 1.0 mm by an alternating current (AC) impedance method (HIOKI 3522-50 LCR Hi-TESTER, Japan) with the electrode diameter of 6.0 mmϕ in the frequency range of 4–100 kHz.

Results and Discussion

Amorphous State

Figure 1 shows the appearance of the fabricated precursor glasses. Na2NiP2O7 showed a rust-red color and high transparency. However, the other samples showed a black color, and only the Na2Fe0.25Ni0.75P2O7 exhibited low transparency. XRD patterns of the bulk and powder, which was pulverized from bulk by an agate mortar of the obtained samples, are shown in Figure 2. All samples showed the typical halo patterns of amorphous with no crystallization.


Figure 1. Appearance of the fabricated Na2FexNi1−xP2O7 glasses.


Figure 2. XRD patterns of the fabricated Na2FexNi1−xP2O7, (A) bulk; (B) powder.

Density Measurement

Figure 3 shows the density result of the fabricated glasses. So we can see that as the x (FeO content) increasing, the density of the glasses tends to be decreasing as a straight line, owing to the molecular weight of FeO is smaller than that of NiO. Figure 3 also shows the calculated theoretical density of the Na2MP2O7 (M = Ni, Fe) crystal in Figure 3. So we can see that the density of Na2NiP2O7 glass is about 97.9% of Na2NiP2O7 crystal, and the density of Na2FeP2O7 glass is about 95.2% of Na2FeP2O7 crystal. The two unparallel lines of the glass and crystal densities changes indicated that there was a little part of oxidized Fe3+ existed in the glass. Because Fe3+ ions are more natural to form tetrahedral configuration, so the real density of Na2FeP2O7 glass is smaller than the theoretical value with all Fe2+ hexahedral configuration. By the way, for the existing of Fe3+, the glasses were fabricated easier, and the network of the glasses will be more stable. Such behavior can be confirmed in the process of glass fabrication (Hirose et al., 2008; Honma et al., 2010).


Figure 3. Density of the fabricated Na2FexNi1−xP2O7 glass and Na2MP2O7 (M = Ni, Fe) crystal.

Crystallization Mechanism

Figure 4 shows the DTA curves of bulk and powder of the obtained samples. The endothermic dips suggest the glass transition temperature (Tg), and the exothermic peaks suggest the glass crystallization temperature (Tp). The crystallization onset temperature (Tx) is also shown in Figure 4. However, we can see that there is a considerable crystallization behavior difference between bulk and powder of Na2FeP2O7 from the DTA results. Because the shape of the DTA pattern is sensitive to the oxidized surface area of the bulk and powder, the Tg and Tx of the glass powder are much higher than those of the bulk glass.


Figure 4. DTA curves of Na2FexNi1−xP2O7 glass, (A) bulk; (B) powder.

The heat-treatment temperature was depended on the glass crystallization temperature (Tp) of the powder, so the heat-treatment was performed on 544, 548, 564, 589, and 610°C. The XRD patterns of that are shown in Figure 5. Na3.12Fe2.44(P2O7)2 (Angenault et al., 1995) crystal was obtained from the Na2FeP2O7 and Na3.14Ni2.18(P2O7)2 crystal (Erragh et al., 2000) was obtained from the other composition of Na2FexNi1−xP2O7 (x = 0.75, 0.5, 0.25, and 0). The simulated patterns of the two kinds of crystals are also shown in Figure 5, which with no other crystal phase precipitated.


Figure 5. XRD patterns of heat-treated Na2FexNi1−xP2O7 glass-ceramics with CB.

In order to analyze the Na2NiP2O7 crystalline phase in the mixture of Na2NiP2O7 glass-ceramics and CB, Rietveld refinement on the powder XRD pattern was performed, and the result is shown in Figure 6. According to the Na3.14Ni2.18(P2O7)2 crystal structure, which is shown in Figure 7, the group of PO4(tetrahedral), NiO6(octahedral), and FeO6(octahedral) units combine by corner-sharing to provide a stable three-dimensional framework to support the de-insertion along the (100) direction of sodium ions. Two types of Ni-Fe substitution were discussed, basing on the position of the Ni atoms. The image of type 1 is shown in Figure 7A, which suggests that the Ni-Fe substitution occurred in the NiO6 units. Besides, the image of type 2 is shown in Figure 7B. It suggests that Fe substituted a part of Ni in the Na (1) sites, which contained about 80% Na and 20% Ni. Owing to the two kinds of substitution type could not be decided which one was main, so lattice parameters were analyzed out by Rietveld refinement.


Figure 6. XRD pattern and Rietveld refinement for the mixture of heat-treated Na2NiP2O7 and CB.


Figure 7. Crystal structure of Na2FexNi1−xP2O7, (A) Ni-Fe substitution type 1; (B) Ni-Fe substitution type 2. Na (yellow), Fe (blue), Ni (green), P (purple), O (red).

We summarized the lattice parameters of the crystalline phase as shown in Table 1. It also shows clearly in Figure 8 that with the Fe substitution increasing, a, b, c axes, and volume were going up at the same time. However, alpha, beta, gamma did not exhibit any component dependency. Because the ionic radius of Fe2+ is larger than that of Ni2+, so the Ni-Fe substitution existed in the Na2NiP2O7 crystal. Since the Ni-Fe substitution type 1 has a significant influence on the crystal structure, it could be the primary way of Ni-Fe substitution. When the lattice parameters (a, b, c) increased by Ni-Fe substitution, the crystal volume got larger than before, and it will be advantaged for the de-insertion of sodium ions.


Table 1. Lattice parameters of crystallized Na2FexNi1−xP2O7 glass-ceramics.


Figure 8. Lattice parameters of crystallized Na2FexNi1−xP2O7 glass-ceramics.

We did the heat-treatment between Tg and Tx on the Na2FeP2O7 and Na2NiP2O7 bulk glasses and observed the crystallization behavior by SEM. Figure 9 shows the SEM images of a fracture surface of the samples crystallized by heat treatment. The same crystallization behavior can be observed that both Na2FeP2O7 and Na2NiP2O7 bulk glasses prefer to develop the crystalline phase on the glass surface. Surface crystallization can lead to high crystal orientation, so such outstanding crystallization behavior is expected to improve the ionic conduction of cathode materials (Akatsuka et al., 2018). Another aspect, the Na2NiP2O7 glass exhibits thermal instability because the ΔT (Theat−treatmentTg) is only 8°C. Hence, we obtained more thick surface crystallied architecture in Na2NiP2O7 rather than Na2FeP2O7.


Figure 9. The section SEM image of (A) Na2NiP2O7 heat-treated at 500°C for 3 h; (B) Na2FeP2O7 heat-treated at 430°C for 3 h.

Electrochemical Properties

The result of the first and second charge-discharge curves of the Na2FexNi1−xP2O7 glass-ceramics is shown in Figure 10A. The initial discharge capacity of Na2FexNi1−xP2O7 from x = 0 to 0.75 were 14.6, 21.8, 31.4, and 57.6 mAh/g. Each one was lower than that of Na2FeP2O7 (68.7 mAh/g). It indicated that with the Fe content increasing, the discharge capacity would be going up. In other words, it will be active with the Fe substitution increasing.


Figure 10. (A) 1st and 2nd charge-discharge curves; (B) dQ/dV plots at 1st and 2nd cycles of the Na2FexNi1−xP2O7 glass-ceramics.

Furthermore, all the flat potential 3.0 or 2.5 V exhibited in the discharge process derived from the reduction of Fe3+/2+ (Honma et al., 2012). However, the flat potential of Ni3+/2+ did not exhibit in any composition. Even in the discharge process of Na2Fe0.25Ni0.75P2O7, there was only a 2.0 V flat potential of Fe3+/2+, suggesting the overvoltage caused by the inactive Ni existing.

To check the redox peaks in the process of charge and discharge, dQ/dV plots that transformed from the charge-discharge curves are shown in Figure 10B. In the 1st charge-discharge process of Na2NiP2O7, there was none redox peak exhibited out, which showed the same result with Zhang et al. (2017). However, in the 2nd charge process, there was an oxidation peak of Ni2+/3+ at about 4.6 V (Zhang et al., 2017) exhibited. In addition, in the discharge process of Na2Fe0.25Ni0.75P2O7, despite there could be a weak electrolytic solution decomposition potential at about 4.3 V, it still exhibited the potential of Ni3+/2+ at about 4.3 and 4.4 V. As a result, Na2FexNi1−xP2O7 with the Fe substitution up to x = 0.25 will activate the Ni3+/2+. However, in total, Ni3+/2+ in the composition of Na2FexNi1−xP2O7 exhibited inactivity.

To know the electrical conductivity of the positive electrode materials, we decided to measure their electrical resistance from 100 to 220°C. Considering the difference of crystallization behavior between bulk and powder, we chose to press the precursor glass powder as a pellet and then measured the electrical resistance of the pellets after heat-treatment under Tp. Figure 11 shows Nyquist plots of crystallized Na2FexNi1−xP2O7 pellets. The intersection of semicircle and horizontal axis determined the electrical resistance, so with the Fe substitution increased, the electrical resistance would be decreased. In other words, electrical conductivity would be increased. However, there was a result that the electrical resistance of Na2Fe0.25Ni0.75P2O7 pellet was higher than that of the other components, which could confirm the same result exhibited in charge-discharge curves. Because of the exceptional electrical resistance exhibited in the composition of Na2Fe0.25Ni0.75P2O7, so the reduction of Fe3+/2+ would be alleviated. With the alleviating of Fe3+/2+, the reduction peaks of Ni3+/2+ which could be activated by the substituted Fe2+ exhibited out. However, the reduction peaks of Ni3+/2+ disappeared at the composition x = 0.5 and 0.75. It may be owing to the active Fe3+/2+ reduction reaction is dominant so the Ni3+/2+ reduction reaction will be unavailable.


Figure 11. Nyquist plots of heat-treated Na2FexNi1−xP2O7 pellets at 220°C.

No matter which kind type of Ni-Fe substitution, it will increase the electric conductivity (Sanz et al., 2001) so that the Ni2+, which surrounds the substituted Fe2+, will be activated. Also, carbon-coatings will enhance the electrochemical behavior of the materials contained Fe (Wang and Sun, 2012), which can ensure a better charge-discharge cycle. However, the liquid electrolyte 1 mol/L EC: DEC [1:1 (vol%)]-NaPF6 showed a decomposition potential at about 4.3 V. It could influence Ni3+/2+ redox so that Ni3+/2+ which has the higher potential (Zhang et al., 2017) did not exhibit out before 4.9 V. Because of the limitation of the liquid electrolyte, seeking the electrolyte with high decomposition potential is necessary.


In conclusion, the Na2FexNi1−xP2O7 glasses were prepared by the melt-quenching method successfully. Moreover, the precursor Na2FexNi1−xP2O7 glasses were confirmed that they contained a part of Fe3+, which was oxidized from Fe2+. Na3.14Ni2.18(P2O7)2 crystal which was obtained from heat-treated Na2FexNi1−xP2O7 glass-ceramics, mainly with type 1 Ni-Fe substitution. With the Fe substitution increasing in the Na3.14Ni2.18(P2O7)2 crystal, it performed a higher activity. In the composition of Na2Fe0.25Ni0.75P2O7, the reduction peaks of 4.3 and 4.4 V appeared in the discharge process. Although reversible charge-discharge reaction could not confirm due to interference with electrolyte oxidation, application to oxide all-solid-state batteries is expected to expand to batteries with higher energy density than sodium iron phosphate derived all-solid batteries.

Data Availability Statement

The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation, to any qualified researcher.

Author Contributions

YJ demonstrated all experiments in the study. TH proposed glass-ceramic cathode for sodium ion battery. TK proposed the preparation of glass-ceramics and the analysis of surface crystallization.


This study was financially supported by JSPS KAKENHI Grant Number JP19K22046 and JP19H02428.

Conflict of Interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.


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Keywords: glass-ceramics, crystallization behavior, sodium-ion batteries, cathode materials, charge-discharge test

Citation: Ji Y, Honma T and Komatsu T (2020) Crystallization of the Na2FexNi1−xP2O7 Glass and Ability of Cathode for Sodium-Ion Batteries. Front. Mater. 7:34. doi: 10.3389/fmats.2020.00034

Received: 30 September 2019; Accepted: 30 January 2020;
Published: 19 February 2020.

Edited by:

Ashutosh Goel, Rutgers, The State University of New Jersey, United States

Reviewed by:

Shi-Xi Zhao, Graduate School at Shenzhen, Tsinghua University, China
Balaji Rao Ravuri, Gandhi Institute of Technology and Management (GITAM), India

Copyright © 2020 Ji, Honma and Komatsu. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Tsuyoshi Honma,

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