Lithium-ion batteries based on intercalation compounds have dominated the advanced portable energy storage market. The positive electrode materials in these batteries belong to a material group of lithium-conducting crystals that contain redox-active transition metal and lithium. Materials without lithium-conducting paths or lithium-free compounds could be rarely used as positive electrodes due to the incapability of reversible lithium intercalation or the necessity of using metallic lithium as negative electrodes. These constraints have significantly limited the choice of materials and retarded the development of new positive electrodes in lithium-ion batteries. Here, we demonstrate that lithium-free transition metal monoxides that do not contain lithium-conducting paths in their crystal structure can be converted into high-capacity positive electrodes in the electrochemical cell by initially decorating the monoxide surface with nanosized lithium fluoride. This unusual electrochemical behaviour is attributed to a surface conversion reaction mechanism in contrast with the classic lithium intercalation reaction. Our findings will offer a potential new path in the design of positive electrode materials in lithium-ion batteries.
As lithium-ion batteries approach the energy density ceiling permitted by conventional intercalation compounds, high demand has arisen for new electrode materials1,2,3. The discovery of a positive electrode—a key performance component of lithium-ion batteries—with high energy/power density, low cost, and long cycle life will expedite progress in emerging areas such as electric vehicles and large-scale energy storage systems. Intercalation-based positive electrode materials contain transition metal ions (preferably early 3d metals) as redox-active elements and lithium ions as charge carriers. Lithium ions diffuse in and out of the material during battery cycling, and thus the host should contain intrinsic lithium conduction paths. Generally, positive electrodes donate lithium ions in lithium-ion batteries, since metallic lithium and lithium-containing negative electrode materials present safety concerns and are chemically unstable4,5. Accordingly, the most commonly explored positive electrode materials are lithium-containing transition metal compounds with a so-called one-, two- or three-dimensional open structure, such as olivine (LiMPO4; M = transition metal), layered (LiMO2), or spinel (LiM2O4) materials6,7,8. Unfortunately, these material groups constitute only a tiny fraction of the existing redox-active transition metal compounds in nature. Numerous transition metal oxides, sulfides, phosphates and nitrides exist, some of which may exhibit suitable electrochemical potentials versus lithium as a positive electrode, which have been ignored since they are lithium-free or contain no lithium conduction path. Alleviating these restrictions would offer unexplored opportunities to identify new positive electrodes for lithium-ion batteries.
Here, it is shown that transition metal monoxides (MO, M = Mn, Fe, Co) that do not contain either intrinsic lithium or a lithium conduction path in their structure can nonetheless function as high-capacity positive electrode materials. These transition metal monoxides are known to be electrochemically active only in negative electrodes (lower than ∼1 V versus Li+/Li) by the conversion reaction9. We demonstrate herein that when they are blended with nanosized lithium fluoride (LiF) in the electrode, they not only donate lithium ions to the negative electrode but also exhibit an average voltage of over 3 V (versus Li+/Li), functioning as a positive electrode. This study focuses on MnO, although characteristics of FeO and CoO are also introduced. This new energy storage mechanism, investigated through a combination of experiment and first-principles calculation, expands our current understanding and brings a variety of unexplored materials into consideration as positive electrode materials.
LiF–MO nanocomposite as positive electrode
Mixtures of LiF and MO (M = Mn, Fe, Co) were fabricated using a high-energy ball miller under an argon atmosphere (Fig. 1a). The presence of the mixture (LiF and MO) was confirmed using X-ray diffraction (Fig. 1b) without any impurity phase, which may be formed during the mechanochemical mixing (Supplementary Figs 1 and 2)10. The particle size of the composite was around 8 nm as shown by high-resolution transmission electron microscopy (TEM) (Supplementary Fig. 3). The mechanochemically treated MnO/C composite was synthesized for comparison with the LiF–MnO nanocomposite to verify the effect of the lithium compound (LiF).
LiF–MO (M = Mn, Fe, Co) nanocomposites showed positive electrode properties with high voltage and capacity after the first charging step (Fig. 2). Almost 0.9 of the lithium in the LiF–MnO nanocomposite participated in the reversible reaction (theoretical capacity corresponding to one lithium: 262.63 mAh g−1) at a 3.1 V average voltage. Meanwhile, the MnO/C composite was nearly inactive in the voltage range >1.5 V and had electrochemical activity only as the negative electrode from the conversion reaction within a low voltage range (<1.0 V) (Supplementary Fig. 4)9,11,12,13. This implies that the addition of LiF critically affects MnO activation during the electrochemical reaction. The characteristic profile of LiF–MnO is displayed in a full cell with Li4Ti5O12 negative electrode (Supplementary Fig. 5)14. LiF–FeO and LiF–CoO nanocomposites delivered discharge capacities of 310 and 206 mAh g−1, respectively, demonstrating the general applicability of metal oxides used as positive electrodes when mixed with LiF (Fig. 2b,c).
Electrochemical response of LiF–MnO nanocomposites
Pseudocapacitive electrochemical behaviour was observed in LiF–MnO nanocomposite from the electrochemical response in the cyclic voltammetry (CV) experiment from 0.075 mV s−1 to 1.00 mV s−1. In the CV experiment, the redox reaction appeared mainly at 2.5 V and 3.75 V, which could be ascribed to manganese redox reaction (Fig. 3a). Cathodic and anodic peak currents at each reaction voltage (2.5 V, 3.75 V) tend to increase as the scan rate increases from 0.075 mV s−1 to 1.00 mV s−1. The redox peak currents obey a power-law relationship with the scan rate, which exhibits a nearly linear proportionality of ip = avb(b = ∼1) (Fig. 3b,c), indicating that the electrochemical reaction is primarily surface controlled in contrast to the bulk-diffusion-controlled reaction (b = 0.5) generally observed in intercalation-based positive electrodes15. The current can be expressed more precisely as the sum of the surface-controlled and diffusion-controlled capacities at a fixed potential16,17,18:
In equation (1), the k1v and k2v1∕2 terms indicate the surface- and diffusion-controlled contributions, respectively. The k1 and k2 values at fixed potentials were determined by the correlation between the scan rates and corresponding current signals according to equation (2) (Supplementary Fig. 6):
Accordingly, the capacitive contribution as a function of the voltage could be obtained using i(V) = k1v at 1 mV s−1 scan rate, as demonstrated in Fig. 3d. The capacity from the surface-controlled reaction accounts for 94% of the overall capacity by comparing the shaded region with the total area. The remarkable power capability of the LiF–MnO nanocomposite ensures the surface-controlled reaction kinetics. The electrode exhibited 110 mAh g−1 discharge capacity even at a current rate of 5,000 mA g−1, with a cycle life stable over 100 cycles (Supplementary Fig. 7).
Mn redox reaction aided by the fluorine ions
The reversible change in the Mn oxidation state was observed during the entire charge and discharge reaction using in situ X-ray absorption near-edge structure analysis (XANES), shown in Fig. 4a,b. Mn oxidation and reduction were evident for both the first and subsequent cycles (Fig. 4c,d). Raman spectroscopy also showed the reversible Mn redox reaction. The stretching bond strength between Mn and O (610–648 cm−1) changed due to variations in the electrostatic attraction force, according to the oxidation and reduction of Mn ions (Supplementary Fig. 8). Similarly, the LiF–FeO nanocomposite also showed that the Fe redox reaction participated in the electrochemical reaction as confirmed by in situ XANES (Supplementary Figs 9 and 10).
As with the reversible oxidation and reduction of Mn, the Li and F ions in LiF participate as charge carriers and charge neutralizers. Additional experiments excluding any fluorine sources other than LiF, that is, using fluorine-free binder and electrolyte, were carried out in Supplementary Fig. 11, which showed no significant changes in the electrochemical profile, confirming the role of LiF as the source of F. X-ray photoemission spectroscopy (XPS) of the Li 1s region showed that the lithium signal at 56.0 eV disappears at charge and is recovered at discharge (Fig. 4e). Especially notable is that the extraction of lithium ions during the first charge indicates the decomposition of LiF. In the F 1s region shown in Fig. 4f, the binding energy of 685.3 eV from LiF increased to 686.0 eV after charge and returned to the initial state when discharged. A peak at 686.0 eV comes from the local environment of the F− ion bound to the Mn ion to satisfy charge neutrality as oxidation occurs.
The electrochemical reaction between the MnO and F ions was further investigated using soft X-ray absorption spectroscopy (Fig. 4g). Mn L-edge signals collected from the surface-sensitive total electron yield mode revealed the characteristic peak of Mn2+ (639.6 eV), including a small portion of the Mn3+ signature in the as-prepared state, which has been observed in MnO in many previous works19. On charging, the Mn3+ and Mn4+ signals increased at the expense of the Mn2+ signal. The reversible change was observed during the subsequent electrochemical cycling, which indicates that not only Mn2+/Mn3+ but also Mn3+/Mn4+ redox reactions are involved in the electrochemical reaction. It was noted that the Mn3+/Mn4+ reaction mainly participates in the high potential redox reaction (∼3.75 V), while the Mn2+/Mn3+ redox reaction occurs in the entire voltage range as described in Supplementary Fig. 12.
The F K-edge spectra revealed slight changes in the 685–687.5 eV range (Supplementary Fig. 13). In the charged state, the peak at 685–687.5 eV, which is mainly observed in the manganese fluoride system (MnF2 or MnF3), slightly increased20. In contrast to the charged state, the peak reversibly decreased in the discharged state. The XPS and X-ray absorption spectroscopy (XAS) results imply that the Mn2+/Mn3+ and Mn3+/Mn4+ redox reactions mainly occur on the MnO surface accompanying F− ion interaction. It is noted that the redox peak at 3.75 V in the CV experiment (Fig. 3a) accompanies the Mn3+/Mn4+-related redox reaction as shown in Supplementary Fig. 12. Additionally, the pseudocapacitive behaviour may be due to the surface redox reaction of MnO with the F− ion from LiF. However, the current response does not establish the reaction mechanism; therefore, we further investigated the reaction mechanism using TEM21.
Surface-concentrated chemical and structural changes
The chemical distribution information for the charged and discharged states was obtained using scanning TEM coupled with electron energy-loss spectroscopy (STEM–EELS) spectrum images (Fig. 5a,b). We minimized the electron beam dose with optimized conditions (Supplementary Fig. 14). We observed both Mn and F signals from the charged and discharged states and confirmed that the F− ion distribution was not homogeneous but preferentially occurred on the MnO surface. It was generally observed that the fluorine distribution was mainly concentrated on the surface of the particle with approximately 2–5 nm thickness regardless of the charge and discharge state for most of the particles, which indicates that the electrochemical reaction with fluorine occurs relatively homogeneously on the surface of the electrode material (Supplementary Fig. 15). This trend is different from that for the iron-based oxyfluoride phase, which has a core/shell structure with an O-rich shell and a F-rich core22. F coexists with Mn in the surface region in the charged state; however, they tend to exist separately in the discharged state. This result is possibly due to the reversible interaction between Mn and F during electrochemical cycling. Therefore, we compared the valence of Mn in the F-rich shell and F-less core region to clarify the reversible interaction between Mn and F (Fig. 5c,d). A significant change in the Mn L3 peak energy was observed in the Mn L2,3 EELS spectra in the charged state. The Mn L3 peak observed for the F-rich shell (641.0 eV) has a higher value than 639.8 eV for the F-less core; however, the peak energies from both the shell and core regions were similar in the discharged state. The non-uniform Mn valence distribution across the single particle in the charged state supports the surface-concentrated Mn redox reaction (Supplementary Fig. 16). This finding indicates that the F− ion incorporation accompanying the redox reaction of Mn ions mainly occurs on the MnO surface.
On charge, significant local structure evolution was observed including attenuation of the rock salt signature and a decrease of the bond distance from in situ extended X-ray absorption fine-structure (EXAFS) analysis (Fig. 5e). X-ray diffraction analyses of the electrode materials do not provide insight into the nature of charged/discharged product due to the loss of long-range ordering during the first charge (Supplementary Fig. 17). Meanwhile, EXAFS showed evident local structure changes during electrochemical cycling. The signal at longer distances (4–6 Å) gradually decreased at initial charging, indicating a reduction in crystallinity. In addition, the electrode undergoes a decrease of bond distances at the first and second neighbour. The shortened bond distance of the first neighbour at charge is similar to manganese compounds, which have a higher oxidation state than Mn2+ (Supplementary Fig. 18). At the end of charge, the electrode showed completely different local structure from the pristine state with the attenuated second neighbour23,24,25,26. This amorphization and attenuation of the rock salt phase signature were similarly observed in the iron oxyfluoride system during the phase transformation from rock salt to the F-rich rutile phase when fluorine interacts with the rock salt phase through the reconversion reaction26. However, the charged state of the LiF–MnO nanocomposite exhibits a distinct local structure from the rutile-type manganese fluoride phase and retained the cubic local structure similar to the MnOx phase (Supplementary Fig. 18).
The reversible recovery of the local structure as the rock salt phase was demonstrated after the discharge. The electrode at the end of discharge exhibits similar features to those of the pristine electrode in the local range of 1–6 Å. The first and second neighbour recovered similarly to those in the as-prepared MnO, and the peaks in the 4–6 Å range reemerged, implying the reformation of the MnO-like crystal structure. The local structure of the discharged state was well matched with the standard rock salt phase MnO model, suggesting that the structural transition is reversible during electrochemical cycling (Fig. 5e and Supplementary Fig. 19). This reversible behaviour was observed continuously during the subsequent electrochemical cycling.
A reversible local structure change was observed on the MnO surface in high-resolution high-angle annular dark-field images (Fig. 5f,g). The atomic-resolution image of the charged state reveals the different atomic structure in the F-rich shell region compared with that in the F-less core region. The fast Fourier transformation (FFT) image of the core region reveals a periodic pattern projected to the [01̄1] zone axis of Fm3̄m MnO, which indicates that the core region is well maintained as the MnO phase. Meanwhile, an additional pattern with a large d-spacing (5.02 Å) was observed in the shell region. The local structure is analogous to the I41∕amd space group Mn3O4 structure considering the crystallographic orientation [01̄1] zone axis of Fm3̄m MnO, which is coherent with the  zone axis of the I41∕amd space group Mn3O4 (Supplementary Fig. 20). However, the surface structure was defectively formed, including a vacancy on the Mn tetrahedral site of Mn3O4 (Fig. 3f). This result may be due to the instability of Mn3+ or Mn4+ ions in tetrahedral sites compared with octahedral sites considering the oxidized environment of the surface region by F− ion incorporation27,28. This face-centred cubic to body-centred tetragonal phase transition is known for the diffusionless transformation29, which indicates that the transformation kinetics could be sufficiently fast to accommodate the high current density during the electrochemical cycling (Supplementary Fig. 7). Given the coherent distribution of the structure transformed region and F− ions (Fig. 5a and Supplementary Fig. 21), the surface local structure of the charged state is expected to be a defective Mn–O–F-type spinel-like phase. In contrast to the charged state, the discharged electrode exhibited a uniform structure even in the shell region as the MnO rock salt phase (Fig. 5g,h and Supplementary Fig. 22).
This reversible structure evolution is identical to the results from in situ EXAFS. As the thickness of the shell region is approximately 2–4 nm (Fig. 5a,f), if we assume the particle size of MnO as 10 nm, the surface layer occupies 78.4% of the MnO single nanoparticle (Supplementary Fig. 23). Therefore, the local structure change from the in situ EXAFS can be originated from the structure evolution on the MnO surface considering the particle size level.
Particle size effect on electrochemistry
Simple numerical calculations, assuming the involvement of the Mn redox reaction up to 2 nm from the MnO surface, confirm the feasibility of a large capacity (>236.37 mAh g−1) for submicrometre-scale particles (∼10 nm). On the basis of the simplified model from the first-principles calculations, the capacity could be numerically predicted as a function of the particle size of MnO (Supplementary Figs 24–27 and Supplementary Text). In particular, the large capacity from the surface reaction was feasible because of the two-electron reaction of the Mn ion (Mn2+/Mn3+ and Mn3+/Mn4+) on the MnO surface (Supplementary Fig. 26). In the simulation, we observed that the capacity can be dramatically increased as the particle size decreases below 10 nm because of the larger surface area of the small-particle electrodes compared with large-particle ones. Our experimental results for the capacity (∼240 mAh g−1) with ∼10-nm particle sizes match with the capacity predicted on the basis of the numerical simulations (Supplementary Fig. 27).
The particle size effect of the metal compound on the electrochemical activity in the nanocomposite cathode material was verified with systematic control of the particle size and shape of manganese oxide (Fig. 6a and Supplementary Fig. 28). Mn3O4 was selected as the metal oxide compound to compare the electrochemical activity as a function of particle size. A LiF–C/Mn3O4 nanocomposite electrode was fabricated by making a mixture with LiF–C and as-synthesized Mn3O4 nanoparticles without additional high-energy ball milling30. LiF and Mn3O4 were well mixed in the carbon matrix without a change in particle size or morphology (Fig. 6b and Supplementary Fig. 29). The LiF–C/Mn3O4 mixture exhibited electrochemical activity as a cathode material with a 3.5-V average voltage redox reaction after the first charge (Supplementary Fig. 30). The capacity increased from 96 to 159 mAh g−1 as the particle size decreased from 20 to 6 nm (Fig. 6c). This result indicates that the particle size of Mn3O4 directly affects the capacity of the LiF–C/Mn3O4 nanocomposite cathode and implies that the particle size of metal compounds can be a feasible tool for tuning the capacity in the nanocomposite cathode material system.
Therefore, the reaction mechanism of the LiF–MnO nanocomposite can be called a ‘surface conversion reaction’, which is described as follows:
The surface conversion reaction (MX + LiA ↔ MX–A + Li) can take advantage of the high-valence redox reaction of transition metals because the capacity of the LiF–MO nanocomposite is fully utilized based on the M2+/M3+ or M3+/M4+ redox reaction. The transition metal is always housed by the anion (by the X anion in the discharged state or by X and A anions in the charged state) in this reaction and can thus maintain the high-valence state offered by the anions and the high-voltage operation of the electrode. LiF functions not only as a Li source for cathode materials but also as an anion source for charge compensation when the oxidation and reduction of a transition metal ion occur. LiF can be regarded as a stabilizer of the oxidized Mn3+ (or Mn4+) ion by providing F− ions from the MnO perspective. In addition, the MnO can be regarded as an assistant that promotes the decomposition of LiF. LiF is difficult to decompose electrochemically by itself because it is a stable ionic compound with a substantially large formation energy corresponding to 6.10 V versus Li+/Li (Supplementary Table 1). It is expected that the electrochemical activity of the LiF–MnO nanocomposite originates from a series of reactions in which a slightly oxidized Mn(2+δ)+ ion is formed by the extraction of an electron during the initial charge, followed by the decomposition of LiF. Therefore, LiF can donate the F− ion to stabilize the oxidized Mn ion of Mn3+ or Mn4+ when it decomposes. This process can occur only when LiF and MnO compounds are intimately well mixed on the nanoscale.
We found that the reaction mechanisms of LiF–MO (M = Fe, Co) nanocomposites are different compared with the case of LiF–MnO. (See Supplementary Information for details.) Both LiF–MO (M = Fe, Co) nanocomposites showed electrochemical activity based on the M2+/M3+ redox reaction, which was enabled by the interaction with fluorine ions. However, the specific fluorine ion behaviour was slightly different depending on the transition metal compound. In the LiF–FeO case, fluorine ions were better incorporated into the host structure due to the thermodynamic stability of the FeOF compound. As a result, this formulation showed remarkably similar electrochemical properties and local structure changes to those of LixFeOF (Supplementary Figs 31–33 and Supplementary Text) during subsequent discharge and charge25,26, similar to our previously reported case of LiF–FeF2, which can be termed a ‘host formation reaction’4. In the case of LiF–CoO, although the trend of change in oxidation state and local structure is similar to the case of LiF–MnO, the changes are relatively small compared with the reversible capacity (Supplementary Figs 34 and 35). It implies that LiF–CoO could have a different charge compensation mechanism including not only Co redox reaction but also other reaction mechanisms, which needs to be revealed by in-depth study as future work. This difference in reaction processes can be determined by whether the fluorinated phase of the initial metal compound occurs. Note that the iron oxyfluoride phase exists, while the manganese or cobalt oxyfluoride phase has not been reported31. The interaction behaviour of the F− ion with metal compounds and the thermodynamic stability of the charged form seem to determine the overall reaction mechanism.
An understanding of this unusual electrochemical reaction behaviour can offer new design criteria for positive electrode materials in lithium-ion batteries. For positive electrode material design, we believe that numerous combinations of transition metal compounds and lithium compounds (other than LiF) are possible, and a variety of redox nanocomposite positive electrodes could be developed with tuning of their electrochemical performances. As long as the transition metal compounds contain a valid redox-active component, anion participation may activate the lithium storage capability regardless of the crystal structure. Also, as the lithium compounds are readily decomposable in the electrochemical cell, it can supply lithium ions in the lithium-ion cells. Moreover, the choice of anions in lithium compounds can be used as an additional rudder to tune the electrochemical properties of the composite electrode.
Synthesis of MnO/C nanocomposite.
MnO/C nanocomposites were synthesized by planetary ball milling (Pulverisette 5; Fritsch). As-received MnO (99%; Sigma-Aldrich) and fluorine-free graphite (Alfa Aesar) were used without further purification. MnO and graphite were inserted into the same container (MnO/C: 1/0.2, w/w) with an argon atmosphere in the glove box. The powders were mixed in the container at 400 r.p.m. for 48 h without rest time.
Synthesis of LiF–MO nanocomposite.
To synthesize the LiF–MO (M = Mn, Fe, Co) nanocomposite, as-received LiF (99.5%; Sigma-Aldrich) and MO (M = Mn, Fe, Co) (99%; Sigma-Aldrich) were used without further purification. Composite material was prepared by planetary milling (Pulverisette 5; Fritsch). LiF, MO (M = Mn, Fe, Co), and graphite (20 wt% of the LiF–MO composite) were inserted into the same container (Li/M = 1.2/1, m/m), and the container was sealed in an argon-filled glove box to minimize air exposure. The inserted powders were homogeneously mixed in the container at 400 r.p.m. for 48 h without rest time to obtain a finely dispersed composite. The synthesized LiF–MO nanocomposite was characterized by X-ray diffraction (XRD) using a D2 PHASER (Bruker) equipped with Cu Kα radiation (λ = 1.54178 Å) at a scanning speed of 0.5∘ min−1 in a 2θ range of 30∘–70∘. Fourier transform infrared and Raman spectroscopy were performed to check the formation of impurities in the amorphous phase.
Synthesis of Mn3O4 nanocrystals.
For the synthesis of Mn3O4 nanocrystals with edge length of 6 nm, 4.9 g manganese (II) acetate tetrahydrate (Aldrich), 53.4 g oleylamine (Acros) and 5.7 g oleic acid (Aldrich) were dissolved in 300 ml of 1-octanol (Aldrich). The mixture were stirred at room temperature over 3 h in a three-necked 1,000-ml flask. The reaction mixture was slowly heated to 120 ∘C in air under magnetic stirring, and before it reached 120 ∘C, 3.8 ml of deionized water was rapidly injected into the reaction solution. The solution was aged at 120 ∘C in air for 2 h. The solution was then cooled to room temperature and washed with acetone and ethanol. The Mn3O4 nanocrystals were retrieved by centrifugation. The ligand exchange procedure using hexamethonium hydroxide solution (HMH; Aldrich) was as follows. First, 0.3 g as-prepared Mn3O4 nanocrystals were dissolved in 10 ml of tetrahydrofuran solution. Second, ∼1 ml of HMH and ∼0.5 ml of deionized water were added to the solution. Then, the nanocrystals were precipitated with ethanol by centrifugation.
For the synthesis of Mn3O4 nanocrystals with edge length of 9 nm, 4.9 g manganese (II) acetate tetrahydrate (Aldrich), 53.4 g oleylamine (Acros) and 2.8 g oleic acid (Aldrich) were dissolved in 300 ml of 1-octanol (Aldrich). The mixture was stirred at room temperature over 3 h in a three-necked 1,000-ml flask. The reaction mixture was slowly heated to 120 ∘C in air under magnetic stirring, and before it reached 120 ∘C, 3.8 ml of deionized water was rapidly injected into the reaction solution. The solution was aged at 120 ∘C in air for 2 h. The solution was then cooled to room temperature and washed with acetone and ethanol. The Mn3O4 nanocrystals were retrieved by centrifugation. The ligand exchange procedure using HMH was the same as that described above for the 6-nm-sized nanoparticles.
For the synthesis of Mn3O4 nanocrystals with edge length of 11 nm, 6.4 g manganese (II) acetate tetrahydrate (Aldrich), 17.4 g oleylamine (Acros) and 3.7 g oleic acid (Aldrich) were dissolved in 390 ml of xylene (Aldrich). The mixture was stirred at room temperature for 3 h in a three-necked 1,000-ml flask. The reaction mixture was slowly heated to 100 ∘C in air under magnetic stirring, and after it reached 100 ∘C, 26 ml of deionized water was rapidly injected into the reaction solution. The solution was aged at 90 ∘C in air for 1.5 h. The solution was then cooled to room temperature and washed with ethanol. The Mn3O4 nanocrystals were retrieved by centrifugation. The ligand exchange procedure was performed using nitrosonium tetrafluoroborate (NOBF4)32; 0.035 g NOBF4 was dissolved in 1.5 ml of dimethylformamide in an Ar atmosphere. This 1.5 ml of NOBF4 solution was then added to the 10 ml of tetrahydrofuran solution of as-prepared nanocrystals. After the ligand exchange process, the nanocrystals were precipitated with hexane by centrifugation.
For the synthesis of Mn3O4 nanocrystals with edge length of 15 nm, 4.9 g manganese (II) acetate tetrahydrate (Aldrich), 53.4 g oleylamine (Acros) and 2.8 g oleic acid (Aldrich) were dissolved in 300 ml of xylene (Aldrich). The mixture was stirred at room temperature over 3 h in a three-necked 1,000-ml flask. The reaction mixture was slowly heated to 90 ∘C in air under magnetic stirring, and after it reached 90 ∘C, 7 ml of deionized water was rapidly injected into the reaction solution. The solution was aged at 90 ∘C in air for 1.5 h. The solution was then cooled to room temperature and washed with ethanol. The Mn3O4 nanocrystals were retrieved by centrifugation. The ligand exchange procedure using NOBF4 was the same as that described for the 11-nm-sized nanoparticles.
For the synthesis of Mn3O4 nanocrystals with edge length of 18 nm, 4.9 g manganese (II) acetate tetrahydrate (Aldrich), 53.4 g oleylamine (Acros) and 2.8 g oleic acid (Aldrich) were dissolved in 300 ml of xylene (Aldrich). The mixture was stirred at room temperature over 3 h in a three-necked 1,000-ml flask. The reaction mixture was slowly heated to 100 ∘C in air under magnetic stirring, and after it reached 100 ∘C, 8 ml of deionized water was rapidly injected into the reaction solution. Then, the solution was aged at 90 ∘C in air for 1.5 h. Thereafter, the solution was cooled to room temperature and washed with ethanol. The Mn3O4 nanocrystals were retrieved by centrifugation. The ligand exchange procedure using NOBF4 was the same as that described for the 11-nm-sized nanoparticles.
For the synthesis of Mn3O4 nanocrystals with edge length of 20 nm, 4.9 g manganese (II) acetate tetrahydrate (Aldrich), 13.4 g oleylamine (Acros) and 2.8 g oleic acid (Aldrich) were dissolved in 300 ml of xylene (Aldrich). The mixture was stirred at room temperature for 3 h in a three-necked 1,000-ml flask. The reaction mixture was slowly heated to 105 ∘C in air under magnetic stirring, and after it reached 105 ∘C, 20 ml of deionized water was rapidly injected into the reaction solution. Then, the solution was aged at 90 ∘C in air for 1.5 h. Thereafter, the solution was cooled to room temperature and washed with ethanol. The Mn3O4 nanocrystals were retrieved by centrifugation. The ligand exchange procedure using NOBF4 was the same as that described for the 11-nm-sized nanoparticles.
Synthesis of LiF–C/Mn3O4 mixture electrode.
LiF–C/Mn3O4 (6, 9, 11, 15, 18, 20 nm) mixture electrodes were fabricated using the following sequence. In total, 70 wt% of the electrode was composed by a mixture of the LiF–C nanocomposite and Mn3O4 nanocrystals (Li/Mn = 1/1 m/m). The LiF–C nanocomposite was synthesized using planetary ball milling (Pulverisette 5; Fritsch). As-received LiF (Sigma-Aldrich) and F-free graphite (Alfa Aesar) were used without further purification. MnO and graphite were inserted into the same container (LiF/C: 1/1, w/w) with an Ar atmosphere in a glove box. The powders were mixed in the container at 400 r.p.m. for 48 h without rest time. In addition, 20 wt% carbon black (Super-P; Timcal) and 10 wt% F-free binder (polyacrylonitrile, PAN) dissolved in N-methyl-1,2,-pyrrolidone (NMP, 99.5%; Sigma-Aldrich) were cast onto aluminium foil using a doctor blade. The NMP was evaporated overnight at 25 ∘C in a vacuum oven. The final portion of active material (LiF/Mn3O4 except carbon) was set as 55.8 wt%.
Test electrodes were fabricated with the following sequence. A slurry of 70 wt% LiF–MO nanocomposite, 20 wt% carbon black (Super-P; Timcal), and 10 wt% polyvinylidene fluoride (PVDF) binder dissolved in N-methyl-1,2,-pyrrolidone (NMP, 99.5%; Sigma-Aldrich) was cast onto aluminium foils using a doctor blade. The NMP was evaporated overnight at 25 ∘C in a vacuum oven. Coin cells (CR2032; Hohsen) were assembled with the LiF–MnO nanocomposite electrode, lithium counter electrode, a separator washed with acetone (GF/F Filter; Whatman), and a 1 M solution of LiPF6 in a mixture of ethyl carbonate/dimethyl carbonate (EC/DMC, 1:1, v/v) in an argon-filled glove box. For XPS measurement, a fluorine-free binder (polyacrylonitrile, PAN) and a 1 M solution of LiClO4 in EC/DMC (1:1, v/v) were used. To evaluate the properties of the LiF–MO nanocomposite, galvanostatic charge/discharge profiles were measured over voltage ranges of 1.5–4.8 V with a potentiogalvanostat (WBCS 3000; WonA Tech) at room temperature. LiF–C/Mn3O4 mixture electrode was tested over voltage ranges of 2.0–4.8 V. The first charge process was performed under the constant current and constant voltage (CC/CV) mode to 4.8 V under 20 mA g−1 at room temperature and maintained until the current density decreased below 10 mA g−1. The capacity was calculated by dividing the absolute capacity by the weight of active material including LiF and MO (M = Mn, Fe, Co). CV measurements were obtained after the first charge using the same protocol as for the galvanostatic charge. The voltage was scanned from 4.8 to 1.5 V as the scan rate was changed from 0.075 to 1.00 mV s−1. The peak currents at 3.75 V and 2.5 V redox reaction were plotted as scan rate and analysed by linear fit in log scale. The adjusted R2 value of 3.75 V was the same as 0.9995 at cathodic and anodic reaction. The values of 2.5 V were 0.9994 and 0.9952 at cathodic and anodic reaction respectively. The standard errors of 3.75 V were 0.00949 and 0.00973 at cathodic and anodic reaction. In the case of 2.5 V, the standard errors were 0.04039 and 0.01579 for each. The full cell was assembled into a coin-type cell with a Li4Ti5O12 electrode as the negative electrode and LiF–MnO nanocomposite as the positive electrode. The cell was tested in the voltage range 0.01–3.3 V at a current rate of 20 mA g−1 based on the weight of the positive electrode.
X-ray absorption spectroscopy and diffraction analysis.
For in situ absorption spectroscopy (XAS) experiments, holed coin cells sealed using epoxy with Kapton film were used. The current rate was fixed at 20 mA g−1, and the charge discharge protocol followed the same conditions as those used in the galvanostatic experiments. In situ XAS was performed at the 7D XAFS and 10C wide XAFS beamlines at the Pohang Light Source-II (PLS-II) using the Si(111) double-crystal monochromator. The beam intensity was reduced by 20%–30% to minimize high-order harmonics. The Mn and Fe K-edge spectra of LiF–MO (M = Mn, Fe) electrodes were recorded in transmission mode at room temperature. The storage ring was operated at 2.5 GeV with a ring current of 100–150 mA. Reference spectra of the Mn and Fe metals were collected simultaneously using Mn and Fe metal foils. The XAS data were analysed using the Athena program, and the spectral energies were calibrated using the first inflection points in the Mn and Fe metal foil spectra. The extracted extended X-ray absorption fine structure (EXAFS) signal, χ(k), was weighted by k3 to emphasize the high-energy oscillations and then Fourier-transformed in a k range from 2.0 to 11.5 Å−1 for the Mn and 2.0 to 11.8 Å−1 for the Fe K-edge using a Hanning window to obtain the magnitude plots of the EXAFS spectra in R-space (Å). Data pre-processing operations such as deglitching, energy calibration, normalization, and least-squares fitting with theory were performed as described in ref. 33 using IFEFFIT34, which used the FEFF code35. Ex situ XRD patterns for the LiF–MnO electrode were collected on the 5A XRD beamline at PLS-II. Samples were prepared by subdividing points in the charge/discharge cycles. Electrodes were collected by disassembling the coin cell after achieving the set capacity. Collected electrodes were washed using diethyl carbonate and dried in a dry room. Samples were sealed using Kapton tape and packed in an aluminium pouch to prevent contamination. The wavelength of the X-ray beam was 0.7653 Å, and XRD patterns were recorded as a set of circles on a Mar 345-image plate detector in the transmission mode for about 1 min of exposure time. The total recording time was about 2.6 min, including the scanning time of the image plate and transfer time of spectral information. The 2θ angles of all the XRD patterns presented in this article have been recalculated to corresponding angles for λ = 1.54 Å, which is the wavelength of the conventional X-ray tube source with Cu Kα radiation for easy comparison with other published results. High-resolution powder XRD data of Mn3O4 nanoparticles were obtained from Beamline 9B at Pohang Accelerator Laboratory (PAL), Republic of Korea. The data were collected over a 2θ range of 10∘–130∘ with a step size of 0.01∘, step time of 6 s, and wavelength of λ = 1.4865 Å.
Near-edge X-ray absorption fine-structure spectroscopy.
NEXAFS spectra of the Mn L3,2-edge and the F K-edge were taken at the 10D KIST bending magnet beamline at the Pohang Light Source-II (PLS-II). All of the measurements were performed at room temperature and the spectra were collected in a total electron yield mode under a base pressure of 3 × 10−10 torr. The spectra were normalized to the incident photon flux, and the energy resolution was 0.1 eV.
Ex situ X-ray photoelectron spectroscopy.
Half-cells of the LiF–MO (M = Mn, Fe) nanocomposites were assembled and electrochemically cycled. The charged electrode was collected by disassembling the coin cell charged to 4.8 V, and the discharged electrode was collected from the coin cell discharged to 1.5 V after being charged to 4.8 V. The collected electrodes were washed using DMC and dried. The chemical states and composition of the collected electrodes were identified by X-ray photoelectron spectroscopy (Thermo VG Scientific).
TEM and STEM–EELS measurements.
For ex situ analysis, electrodes at different states of charge in half-cells were disassembled in a glove box and washed using DMC before drying. The electrodes detached from the aluminium current collector were immersed in DMC and dispersed using sonication. The TEM sample grid was covered by DMC to minimize any exposure to air during the sample transfer and kept in a vacuum before being transferred to the transmission electron microscope36.
STEM–EELS measurements were performed using a cold-field-emission-type Cs-corrected JEM-ARM200F equipped with an EELS detector (965 GIF Quantum ER) installed at the National Center for Inter-university Research Facilities (NCIRF) at Seoul National University. High-resolution annular dark-field images were collected with 0.1-nm spatial resolution. TEM was performed at 80 kV. For STEM–EELS elemental mapping, the energy dispersion was set as 0.25 eV per channel. The full-width at half-maximum of the zero-loss peak in vacuum was 1.0 eV. The convergence and collection semiangles were 19 and 52.8 mrad, respectively. TEM and energy-filtered TEM (EFTEM) images of the as-synthesized Mn3O4 nanoparticles and LiF–C/Mn3O4 electrode were captured using a JEOL-2100F at 200 kV.
The data that support the plots within this paper and other findings of this study are available from the corresponding author on request.
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This work was supported by Samsung Research Funding Centre of Samsung Electronics under Project Number SRFC-TA1403-03. Also, this work was supported by Project Code (IBS-R006-G1). S.-K.J., H.K., K.-Y.P. and K.K. are grateful for the financial support from IBS.
The authors declare no competing financial interests.
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Jung, SK., Kim, H., Cho, M. et al. Lithium-free transition metal monoxides for positive electrodes in lithium-ion batteries. Nat Energy 2, 16208 (2017). https://doi.org/10.1038/nenergy.2016.208
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