Abstract
Lithium iron phosphate (LiFePO4, LFP) is widely recognized as a cathode material for lithium-ion batteries (LIBs) owing to its excellent high temperature stability, environmental compatibility and impressive cycle retention. Nevertheless, the limited lithium-ion migration rate and poor electronic/ionic conductivities of this material restrict its practical application. This review explores different methods for synthesizing LFP, such as hydrothermal, sol–gel, microwave-assisted, and carbon reduction techniques, assessing them in terms of structural control, scalability, and performance. Additionally, it highlights modification strategies that have evolved from traditional carbon coating to more advanced techniques, such as heteroatom doping in carbon layers, the integration of multi-walled carbon nanotubes (MWCNTs), and thin oxide nanoscale coatings. In this review, the advancements in utilization of LFP for conventional LIB applications as well as in all solid state lithium batteries (ASSLBs) are highlighted, pointing toward future directions for high performance and durable energy storage technologies.
Lithium iron phosphate (LiFePO4, LFP) is widely recognized as a cathode material for lithium-ion batteries (LIBs) owing to its excellent high temperature stability, environmental compatibility and impressive cycle retention.
1. Introduction
Lithium-ion batteries (LIBs) are the industry standard for innovative gadgets, handheld appliances, and hybrid or all-electric automobiles owing to their remarkable specific energy and power density properties.1–3 As shown in Fig. 1, lithium ions move through the electrolyte from the cathode to the anode during charging and reverse direction during discharging. The four main components of a standard LIB are an electrolyte, an anode, a separator, and a cathode. The separator, a porous insulating layer, allows the transport of Li-ions while preventing direct electrode contact and short circuits.4
Fig. 1. Schematic of working principle of lithium ion battery during charge and discharge.
Cathode properties largely determine LIBs performance.5 Currently, widely used cathode active components in LIBs are generally divided into three major kinds based on their crystal frameworks (1) olivine framework (e.g., LiFePO4), (2) spinel framework (e.g., LiMn2O4), (3) layered oxide framework (e.g., LiCoO2, LiNiO2, NCA (LiNiCoAlO2), and NCM (LiNiMnCoO2)).6 Li-ion diffusion channels are two-dimensional in layered oxides but three-dimensional in spinel-type oxides, as discovered in 1983 ref. 7. LFP and other olivine-type oxides were discovered in 1997 and have unidirectional lithium ion flow.8Fig. 2 display the crystal frameworks of the three main kinds of Li insertion cathodes.9
Fig. 2. Crystal structures of layered LiCoO2, spinel LiMn2O4 and olivine LiFePO4 cathode materials.9,10 Reproduced from open access article ref. 9 with permission MDPI, copyright 2014.
Therefore, transition metal oxides that include lithium, such as LiCoO2,11 LiNiO2,12 LiMn2O4,13 LiFePO4 (ref. 14) as well as their modified forms, have been extensively researched to create effective cathode materials for LIBs.15 However the layered and spinel oxides generally suffer from safety, stability or cost limitations making olivine type LFP an attractive alternative. Due to its fast charging ability and lifespan consistency, LFP is regarded as a potential cathode material.16 The capability for rapid charging is increasingly regarded as a crucial feature in the advancement of rechargeable energy storage systems, particularly within the realm of electric vehicles (EVs).17 LFP is identified as a pivotal cathode material due to its superior thermal stability, prolonged cycle life, economical, non-hazardous, and reliable performance under high-temperature conditions.16,18,19 Owing to its crystalline structure in bulk and optimum particle size in nanostructure, LFP has a greater charge storage capacity of approximately 170 mAh g−1, enabling good performance even at high discharge rates.20 Nevertheless, its rate capability is hindered by its intrinsically poor electronic/ionic conductivities and weak lithium-ion mobility, low bulk density, which limits its practical applications.21–25 The low-rate capability of LFP makes it extremely difficult to be widely sold as a cathodic active material for LIBs.23 Techniques including particle downsizing, morphological control, cation doping and surface coating have been extensively used to overcome these limitations.26–30 Although doping improves conductivity, its mechanism remains debated, while particle shrinking enhances Li+ ion transport, it also increases surface area which results in reduced bulk density and increased polarization.31–33 One of the most successful approach for improving the electrical mobility and electrochemical stability of LFP is surface coating.34 Although carbon coating has significantly improved the electron transport of LFP, further advancements in charge–discharge performance are being understood through synergistic strategies, including heteroatom doping (e.g., nitrogen and magnesium) metal oxide or nanoscale surface modification and the incorporation of conductive frameworks such as multi-walled carbon nanotubes (MWCNTs).35–38 Beyond enhancing conductivity and stability, these modification techniques are pivotal in overcoming challenges related to scalability and commercialization, ensuring that laboratory improvements can be effectively implemented on a larger scale.39 Recent reports also emphasize the effectiveness of such advanced strategies in improving LFP performance and scalability.40,41 Building on these advances, LFP can also be used with sulfide and composite solid electrolyte which has been demonstrated to improve thermal stability, interfacial stability and ionic conductivity.5 These configurations also enables in situ interface chemistry, polymer electrolytes, stable mixed conducting interface and uniform lithium ion deposition for all next generation solid state batteries.39–44
2. Cathode modification
The primary drawback of LiFePO4 with PO43− polyanions is its inherently low electrical conductivity, which leads to significant polarization during both charging and discharging processes. If its conductive agent is not well distributed, the total capacity of LFP is generally diminished. Additionally, the instability of the electrolyte contributes to a decline in performance. LiPF6, one of the most widely used lithium salts in LIB, is extremely sensitive to moisture, even at very low concentrations. The hydrolysis reaction model of LiPF6 in the battery electrolyte are represented as.45–47
| LiPF6 ⇋ LiF + PF5 | 1 |
| PF5 + H2O → 2HF + POF3 | 2 |
The HF produced in this reaction attacks the LFP surface, LiPF6 can dissolve transition metals and damage the cathode surface. To address these challenges, surface coatings are used as an effective solution.46 Conclusively, the electrochemical stability of LIBs is enhanced, and acidity is mitigated by incorporating nanosized oxide particles into the electrolyte to absorb HF. Additionally, oxide nanoparticles applied to the cathode surface can locally absorb HF, thereby reducing the acidic environment near the cathode and protects the active material.41,48,49
Surface coatings offer several advantages for LFP based cathodes:
(i) Forming an electronically conductive layer that facilitates charge transfer.
(ii) Modifying the surface to improve electrochemical performance and structural stability.
(iii) Functioning as HF scavengers, which decrease electrolyte acidity and shield the cathode from dissolution.50
For example, ZnO and Al2O3 coating layers can react with HF to create stable molecules like ZnF2 and AlF3, which lowers the acid concentration and enhances battery efficiency.51,52
| ZnO + 2HF → ZnF2 + H2O | 3 |
| Al2O3 + 6HF → 2AlF3 + 3H2O | 4 |
These reactions produce protective layers that slow down cathode degradation and improve short term capacity retention. However over long cycling periods, HF scavenger depletes, highlighting the importance of nanoscale coatings with high chemical stability.53 The protective layer maintains the material robustness of the cathode by creating a barrier that reduces undesirable interactions between the electrode and electrolyte (Fig. 3).54
Fig. 3. Effect of surface coating on cathode materials in suppressing side reactions and enhancing structural stability.
3. Synthesis techniques for LFP-based cathodes
Cathode-based materials such as LFP can be created in several ways, including carbon-based reduction, microwave reactions, hydrothermal, and sol–gel methods, which are described below.
3.1. Hydrothermal approach
Hydrothermal synthesis is an effective way for formulating fine particles, providing benefits such as a simple procedure and short energy consumption; unfortunately, the plank-like geometries of the LiFePO4 powders produced via this approach can have negative impacts on the material's chemical and physical characteristics, and by adding PEG (polyethylene glycol) to the original solvent mixture, well-crystallized LiFePO4 particles were obtained using a hydrothermal technique; consequently, a starting capacity of 143 mAh g−1 was attained.55
A microwave assisted hydrothermal approach was used to quickly synthesize LFP at 200 °C in 10 minutes, producing a high purity single phase material without the need of post calcination. The cathode showed a specific of 126 mAh g−1 at 0.1C and a coulombic efficiency of 94–96%, highlighting this route as a fast and energy efficient process for LFP preparation.56 The hydrothermal synthesis of LFP involved the use of urea as a reducing agent, at different temperatures (150–200 °C), and Li precursors (LiCl, LiNO3, LiOH, and Li2SO4). Single-phase LFP forms were characterized using a dissolution–precipitation mechanism at temperatures between 170 and 180 °C and reaction periods greater than 12 hours, conclusively, Li2SO4 produced flower-like agglomerates, while the other precursors produced bulky particles (Fig. 4).57
Fig. 4. FE-SEM micrographs of LFP powders prepared hydrothermally for 12 h with 20 mmol urea and Li2SO4 (Li : Fe : P = 3 : 1 : 1) at different temperatures: 170 °C (a), 180 °C (b), 190 °C (c).57 This figure is adopted/reproduced/reprinted from ref. 57 with agreement from Elsevier, copyright 2017.
The amalgamation of LiFePO4 involved varying the ratio of LiOH to H3PO4, maintaining the acidic or basic nature of the solution at 6.5, and mixing the liquid at a controlled temperature to guarantee homogeneity. The combination was subsequently hydrothermally treated for 12 hours at 180 °C.5,58 A hydrothermal approach was used for LiFePO4 having doped and undoped Mg, as a result, doping imposes minor impact on the LiFePO4 composites electrochemical performance and electronic conductivity.59 Phospho-olivine LFP cathode-based materials were effectively organized through hydrothermal reactions at diverse temperatures. An orthorhombic olivine-type structure with a normal grain size of 200 nm was confirmed by XRD and SEM studies of the sample that was produced at 170 °C and then calcined at 500 °C (Fig. 5), which represented 98% of the hypothetical capacity and had the maximum output storage capacity of 167 mAh g−1 at 0.1C.60
Fig. 5. Cycling stability of LiFePO4 prepared at different temperatures.60 This figure is adopted/reproduced/reprinted from ref. 60 with agreement from Elsevier, copyright 2007.
3.2. Microwave-based method
Microwave processing technology is an innovative thermal treatment method that utilizes the effective absorption and transformation of electromagnetic radiation, and this approach is unique in that it uses a self-heating mechanism, which causes the sample to heat rapidly and continuously inside, frequently at much lower temperatures than with traditional heating techniques.61
LiFePO4 nanorods were rapidly created below 300 °C utilizing microwave-based techniques (microwave solvothermal/hydrothermal), and conductivity was enhanced by carbon coating (in situ with glucose, ex situ with sucrose); also, better battery performance was demonstrated by smaller particles from the MW-ST(microwave solvothermal) technique because of improved electrical conductivity and lithium ions mobility.62 The LiFePO4–C composite was prepared quickly and easily by ball-milling for thirty minutes and then heating it in a microwave for 2–4 minutes. The material displayed fine, homogeneous particle size, equal carbon distribution, and was well-crystallized and free of Fe3+ impurities, this material provided an early-stage discharge capacity of 161 mAh g−1 and showed extraordinary long-term stability at C/10 (Fig. 6).63
Fig. 6. (a) Charge–discharge curve and (b) cycling performance of LiFePO4/C (8.10 : 1 ball milling, 2 min microwave) at 27 °C.63 This figure isadopted/reproduced/reprinted from ref. 63 with permission from Elsevier, copyright 2007.
The effective amalgamation of LiFePO4 involves simple microwave heating without the use of reductive gas flow. By using activated carbon as the microwave absorber, the heat treatment time can be significantly reduced, and the need for any precursor can be eliminated, as it is not a precursor itself. In addition, this procedure is extremely simple, inexpensive, and repeatable. Consequently, we achieved the maximal discharge specific capacity and the optimal stability during cycling at a duration of four minutes of microwave heating.64
Subsequently, a 4-minute microwave heating (Fig. 7), which can be charged with 159 mAh g−1 and discharge with 151 mAh g−1 at room temperature, where the early discharge capacities at C/10, C/2, and 1C rates were 151 mAh g−1,139 mAh g−1 and 134 mAh g−1 respectively, showing good cycle life properties and rate capabilities.64
Fig. 7. SEM Analysis of LiFePO4 particles synthesized by microwave heating for 4 minutes.64 This figure is adopted/reproduced/reprinted from ref. 64 with permission from Elsevier, copyright 2003.
Using microwave processing, LFP with high selective capacity is made from the precursor NH4FePO4·H2O showing a two-phase charging/discharging behavior, maintaining a uniform potential around 3.4 V, and as the heating time increases, the discharge capacity improves, specimen A gives 119 mAh g−1, specimen B (10 min) 134 mAh g−1, specimen C (15 min) 156 mAh g−1 while overheated specimen D drops to 102 mAh g−1, which indicates that these samples are stable over time, however, specimen C performed best even at high current. This implies that 15 minutes of heating provides the best battery performance, even though specimen D has higher conductivity.65
3.3. Carbon-based reduction approach
An economical and environmentally responsible approach for producing LFP/C powders is the carbothermal reduction procedure, which provides precise control over particle morphology and oxidation states, improving surface area, electron transport, and lithium-ion diffusion. A consistent sheet of carbon is created on the particle surface by heating the carbon source with the precursor, greatly enhancing the electrical conductivity and electrochemical performance.5
Wet milling and spray drying carbothermal reduction (WSC) have been used to form a new mesoporous bowl-shaped LFP/C composite. This composite is characterized by pores approximately 13.3 nm in size, an effective area of 29.4 m2 g−1, and primary particles uniformly coated with carbon, each measuring less than 100 nm. It shows a greater storage capacity of approximately 123 mAh g−1 at 10C, maintaining this capacity over 100 cycles without degradation. The exceptional rate performance of this composite is ascribed to enhanced lithium-ion distribution, an expanded reaction surface area, and improved electronic conductivity (Fig. 8).66
Fig. 8. (a) Formation scheme of the mesoporous bowl-like LiFePO4/C morphology and (b) its discharge profiles and rate capability at different current densities.66 This figure being adopted/reproduced/reprinted from ref. 66 with permission from Elsevier, copyright 2003.
Using β-FeOOH nanorods as the initial precursor and glucose as the carbon donor and reducer, a thermal reduction method was used to create the LFP/C composite. The findings indicate that the electrochemical performance of the final LFP/C product is influenced by the amount of carbon and morphology of the starting material. The LFP14 specimen containing 2.79 wt% carbon, exhibited discharge capacities of 158.8, 144.3, 111.0, and 92.9 mAh g−1 at 0.1, 1, 10, and 15C rates, respectively, and regained 157.5 mAh g−1 or 99.2% of its original capacity when the rate was returned from 15C to 0.1C. This highlights that the LFP/C material synthesized by this method offers strong potential for large-scale production and application in LIBs, especially for electric and hybrid vehicles, owing to its excellent cycling durability and negligible drop of capacity after 100 cycles at 0.5C.67
3.4. Sol–gel approach
The sol–gel process was used to control the powder's grain size and improve its electrochemical characteristics. The adipic acid-assisted sol–gel technique was created at 670 °C in an argon environment. There were a few large particles, approximately 200–300 nm in size, mixed with a large number of polycrystalline particles, approximately 50–100 nm in size. At a high current density of more than 30C, the cell showed a high initial discharge capacity beyond 150 mAh g−1 and good cycle performance.68 The sol–gel method was successfully used to create a pure and highly crystalline form of LFP with regulated levels of LiI (lithium Iodide) and carbon covering. LFP's purity and particle size of LFP were significantly affected by the amount of LiI. During cycling, the optimized LFP sample displayed a steady current density and a discharge capacity that was nearly equal to its theoretical value. Also, by creating a cavity-like structure, this carbon coating improved the diffusion and charge transfer of lithium ions.69 In the sol–gel procedure, citric acid was utilized as a carbon precursor to produce both pure LFP and LFP/C. The creation of LFP/C involved the employment of three dissimilar metals to citric acid stoichiometries specifically 1 : 0.5, 1 : 1, and 1 : 2. Among the four samples that were prepared, the consequences showed that LFP/C (1 : 1) had the highest discharge capacity, measuring 148.2 mAh g−1 at a rate of 0.1C and 113.1 mAh g−1 at a high rate of 5C. This was due to its ideal thickness of 4.2 nm and increased graphene-like carbon layer and beyond 300 cycles at a 1C rate, the sample LFP/C (1 : 1) exhibits 96% capacity stability.70 LFP/C sample was synthesized with good performance by a bio-synthetic sol–gel process that used yeast as a bio carbon source. The sample annealed at 800 °C had the best retention (94.3 mAh g−1 at 5C after 100 cycles) and superior discharge capacity (158.3 mAh g−1 at 0.1C) demonstrating its outstanding potential as a high performance cathode material.71 Using a citric acid as a chelating agent and yeast as a template carbon coated LFP samples (LFP@C-1, LFP@C-2, LFP@C-3) were synthesized in a bio assisted sol–gel procedure (Table 1). Among them, LFP@C-3 exhibited the highest discharge capacity (∼157 mAh g−1 at 0.1C) and best rate performance because of its superior electron transport, higher purity and homogeneous carbon coating (Fig. 9).72
Table 1. Merits and demerits of different approaches for making LFP cathode active material.
| Preparation method | Merits | Demerits |
|---|---|---|
| Hydrothermal method | Superior performance (including exceptional rate capabilities (120 mAh g−1 at 10C) and high reversible capacity (up to 163.6 mAh g−1))73 | Requires expensive lithium salt73 |
| Material stability and reduced costs of production74 | High-pressure equipment may be needed and rong reaction times76 | |
| Low energy consumption75 | ||
| Microwave-based method | Efficient heating and brief synthesis duration shorter processing duration77 | Energy consumption. Temperature measurement limitations79 |
| Eco-friendliness78 | ||
| Carbon reduction method | Simple procedure, low cost of manufacturing and low cost of raw materials5 | Stability is difficult to maintain. Mixing is homogeneous, and oxidation problems during drying are common5 |
| Sol–gel method | Good control of particle size, increased surface area and enhanced electrochemical properties performance71 | Challenges in scaling and temperature control80 |
Fig. 9. (a) Initial charge–discharge profiles of synthesized electrode materials at 0.1C and (b) charge–discharge profile of LFP@C-3 at different rates of 0.2C, 0.5C, 2C and 5C.72 This figure is reproduced from ref. 72 with the permission from Elsevier, copyright 2019.
4. Surface degradation and protection mechanism
A well-known and effective technique for safeguarding cathode materials while enhancing lithium-ion surface coating's specific capacity, thermal stability, and electrochemical performance is surface covering. Carbonaceous compounds like reduced graphene oxide (rGO), carbon nanotubes (CNTs), graphene, porous carbon, and graphene are the most commonly utilized covering materials (Fig. 10) because of the following benefits: (1) having excellent stability, both chemically and electrochemically. Carbon materials exhibit electrochemical activity at very low potentials, showing great electrochemical stability and strong defense against corrosion of acid electrolytes, owing to interactions between the electrode and electrolyte. Furthermore, carbon compounds can shield the cathode material from atmospheric oxygen and moisture because they are difficult to oxidize. (2) In addition, carbon has special physical characteristics such as low density, great mechanical strength, structural flexibility, and anisotropic conductivity.81,82 (3) High electrical conductivity. Carbon is a valuable covering material because it is an excellent conductor of electricity. (4) Cost effectiveness. Carbon is readily available, inexpensive, and friendly material. Additionally, by modifying the carbon material and preparation conditions, the thickness and conductivity of the carbon covering can be adjusted.21 Owing to its superior qualities, carbon is frequently considered a good surface-coating material for LIB cathodes. Improving superficial chemical stability, increasing the material's structural stability, and facilitating effective lithium-ion diffusion are the three main advantages of carbon coating. Each of these mechanisms supports and strengthens the other. The carbon layer strengthens the interfacial chemical stability and permits more uniform lithium-ion transport during charge–discharge cycles by reducing the dissolution of transition metal ions and surface imperfections.81,83
Fig. 10. Schematic illustration of cathode behavior with (b) and without carbon coating (a).
5. Performance enhancement approaches of LFP cathodes
5.1. Carbon-based coating for LFP
Conductive materials, namely amorphous carbon, natural graphite, and fibrous carbon, are combined with electrode components to improve electrical pathways since high-rate battery charging and discharging depend on well-organized electron and lithium-ion transfer. However, when the LFP particle size is reduced to the nano or submicron level, more carbon is required to connect the particles, reducing the amount of active substance and thus affecting the energy per unit mass. Challenges, such as achieving uniform carbon distribution, remain, which can be addressed through mechanofusion coating and surfactant-assisted slurry preparation or by combining active compounds with carbon during synthesis to improve conductivity.84
Carbonized LFP and LFP/C composites were made with a variety of LFP precursors and carbon sources, such as stearic acid,85 sucrose, glucose, sugar,86 and resorcinol–formaldehyde.87 The synthesis required heat treatment in an inert environment at temperatures between 500 °C and 800 °C.21 The LFP crystal particles were maintained between 100 and 200 nm in size, and their mass percentage of carbon ranged from 3 to 15%. These materials exhibited outstanding cycle and rate capabilities, as well as a 160 mAh g−1 discharge capacity, demonstrating good electrochemical performance. But even a tiny quantity of carbon (less than 1% mass) was shown to drastically lower the final electrode sheet's density.88 When the carbon concentration reached 31 wt%, the electrical conductivity of the electrode sheet improved by approximately seven orders of magnitude, demonstrating the effectiveness of carbon-coated LFP with sucrose.89 The performance was also improved by the covered layer depth and homogeneity of the carbon covering, as demonstrated by the improved outcomes when more carbon was applied to the carbon-coated LFP particles.90 Carbonized LFP was prepared hydrothermally with glucose as the carbon precursor; the resultant rod-like LFP particles were uniformly sized at about 220 nm, and they were covered in a layer of carbon that was 5–12 nm thick and containing 5 wt% carbon. Excellent cycling and rate performance were demonstrated by these particles.21,91
5.2. MWCNT-based conductive coatings
CNTs are ideal for nanoscale molecular devices because of their small size, great tensile strength, chemical durability, high thermal conductivity, strong sp2 carbon bonds, and special electrical characteristics.92
Later, the insertion of MWCNTs into the carbon coating, their high aspect ratio, three-dimensional structure, and superior electron mobility created a robust conductive network and increased the mechanical strength.93,94 LFP covered with MWCNTs was synthesized via hydrothermal approach, and then subjected to heat treatment. Various characterizations were performed to examine the pure LFP and LFP-MWCNT samples, as shown in Fig. 11a and b.95
Fig. 11. Comparison of the XRD patterns (a) and cyclic voltammetry profiles (b) of the uncoated LFP and LFP/MWCNT composites.95 Both figures (a and b) are reproduced from ref. 95 with permission from Elsevier, copyright 2009.
The LFP-MWCNTs exhibited a superior discharge performance and improved cycling durability in contrast to pristine LFP. Notably, the sample containing 5 wt% MWCNTs demonstrated an initial discharge capacity of 160.3 mAh g−1 at 0.3C, with only 0.4% capacity fading observed upon 50 cycles.95
The effectiveness of applying MWCNTs was tested using three different types of LFP cathode samples: mechano-fusion (MF) dry coating, conventional coating, and the new incipient coating (IC) approach (Fig. 12). The IC technique created a uniform and thin coating layer with minimal material, improving electronic and ionic conduction, lowering internal resistance, and suppresses particle aggregation. As a result, the rate capacity increased by 30% and had a capacity of 157.57 mAh g−1 at 0.1C, as well as outstanding, long-lasting cycling durability, preserving 99.33% of its capacity after 150 cycles at 1C/45 °C.96
Fig. 12. Incipient coating of MWCNTs on LFP enhances electron and ion pathways.96 Reproduced from ref. 96 with permission from the American Chemical Society, copyright 2025.
A nanosized C/LFP/MWCNTs composite produced by hydrothermal and electro polymerization techniques demonstrated outstanding electrochemical performance, delivering 169.9 mAh g−1 at C/10 and 143.4 mAh g−1 at 20 C. After 200 cycles, the formation of a 3D conductive network improved the transportation of both electrons and Li+ ions, resulting in >95% capacity retention.97
5.3. Heteroatom doping in carbon layers
Heteroatom doping in carbon layers has been a successful method for improving LFP cathode electrochemical behavior.98 Heteroatoms like N, S, B, P, and F can be added to the carbon network to enhance electrochemical performance by promoting the diffusion of lithium ions, generating defect sites, and boosting electronic conductivity.99 LFP-based cathodes in LIBs are made more electrochemically efficient by nitrogen-doped carbon surface engineering.38,100–102 N (nitrogen) doping improves electron transport by boosting carrier density, enhancing the interface between carbon and LFP, and forming active sites and surface defects that reduce the energy barrier to ion penetration.101,103 However, excessive nitrogen doping frequently results in the production of thick C–N domains, creating agglomeration in the coating layer and poor high-rate performance. This may be efficiently addressed by utilizing a synergistic doping method that includes both nitrogen and manganese(Mn).38 Dual doping with Mn and N (Fig. 13) increases the ductility of LFP by decreasing microcrack development and minimizing shear deformation, which lessens the barricade of lithium ion transport, promoting quicker ion transport and overall electrochemical performance.104 For LFP particles at the micrometer scale, the LFP/C–N–Mn material demonstrated extraordinary rate capacity and robust cycling behavior (e.g., 119 mAh g−1 at 10C, 88% retention after 600 cycles at 5C) (Fig. 14).38
Fig. 13. (a) Carbon coating on LFP; (b) layer of N-doped carbon on LFP; (c) N–Mn co-doped carbon layer on LFP; and (d) Mn-induced deagglomeration effect.38 Reproduced from ref. 38 with permission from the American Chemical Society, copyright 2024.
Fig. 14. Electrochemical performance of LFP composites: (a) rate performance (0.1–10C); (b) cycling stability at 1C; (c) charge/discharge shapes with voltage plateau inset; (d) cycling at 5C, and (e) charge/discharge profiles of LFP/C–N–Mn (0.1–10C).38 Reproduced from ref. 38 with permission from the American Chemical Society, copyright 2024.
Additionally, the beneficial effects of dual-heteroatom doping, such as N, S co-doping, create a large number of active sites and porous frameworks that improve Li storage and charge transport.105 For instance, the solid state approach of synthesizing N,S doped carbon-coated LFP(NSC-@LFP) with methionine exhibits outstanding performance, providing 155 mAh g−1 at 0.1C and 99% capacity retention after 200 cycles due to better ionic/electronic conductivity and rapid ion diffusion.99 LFP/C composites with F, Mn, Nb, and Mg dopants that were made by ball milling shown superior electrochemical performance were improved (Fig. 15). As a result, Nb enhanced cycling stability (>96% after 100 cycles), Mn increased low temperature capacity (113.7 mAh g−1 at 10C) demonstrating the beneficial effects of elemental doping for LFP/C cathodes.98
Fig. 15. Schematic representation of the carbothermal reduction process paired with a combined bulk phase doping approach to prepare LFP/C cathode materials.98 Reproduced from open access article ref. 98 with permission MDPI,copyright 2024.
LiFe0.98M0.02PO4/C (M = Mg, Ni, Co, Sr) composites were created using a solid-state technique with glucose and Fe2O3 where XRD verified that there were no impurity phases present (Fig. 16), and doping caused changes in unit–cell parameters (Table 2), which led to an enlarged lattice volume that widened the Li+ diffusion channels, improved charge–discharge behavior, and introduced lattice distortions that increased hole formation, which improved electronic conductivity (Table 3), among the dopants, Ni2+ demonstrated the uppermost conductivity (3.11 × 10−3 S m−1) and excellent electrochemical performance, with an initial discharge capacity of 156.6 mAh g−1 at 0.2C and 149.4 mAh g−1 at 1C, respectively, maintaining 98.8% and 97.2% capacity retention after 30 cycles.106
Fig. 16. XRD patterns of LFP samples doped with different metal ions.106 Reproduced from ref. 106 with permission from the John Wiley and Sons, copyright 2013.
Table 2. Features of unit–cells in samples with different dopants.106 Reproduced from ref. 106 with permission from the John Wiley and Sons, copyright 2013.
| Dopant | a/nm | b/nm | c/nm | V/nm3 |
|---|---|---|---|---|
| Undoped | 1.0315 | 0.5962 | 0.4635 | 0.2851 |
| Mg2+ | 1.0317 | 0.5999 | 0.4693 | 0.2905 |
| Ni2+ | 1.0334 | 0.6007 | 0.4697 | 0.2916 |
| Co2+ | 1.0331 | 0.6000 | 0.4702 | 0.2914 |
| Sr2+ | 1.0339 | 0.6009 | 0.4701 | 0.2920 |
Table 3. Electronic conductivities of samples with various dopants.106 Reproduced from ref. 106 with permission from the John Wiley and Sons, copyright 2013.
| Dopant | σ/(S per m) |
|---|---|
| Fe2+ | 5.07 × 10−6 |
| Mg2+ | 7.75 × 10−4 |
| Ni2+ | 3.11 × 10−3 |
| Co2+ | 8.63 × 10−4 |
| Sr2+ | 1.68 × 10−5 |
5.4. Metal oxide and nanosize coating
A variety of metal oxides, such as MgO,107 ZnO,108 Al2O3,109 TiO2,110 ZrO2,111 and SiO2 (ref. 112) are used to modify the surface of LFP based cathode materials.113 Stabilization is essential for preserving the battery's integrity and performance over long cycles, and coatings decrease structural degradation and active lithium loss, which are two prominent attenuation mechanisms in LFP batteries.114 It is believed that aluminum oxide (Al2O3) serve as one of the greatest suitable covering substances for improving the cathode materials' rate capabilities as well as capacity retention in LIBs.109,115 By blocking straight interaction between the electrolyte and the cathode, the Al2O3 covering not only creates a protective CEI (cathode electrolyte interface) layer that lowers irreversible capacity loss and lithium-ion migration resistance, but it also neutralizes HF, safeguarding the electrode and stabilizing the cathode material's bulk structure.116 The wide bandgap (3.7 eV) of amorphous Al2O3 (ref. 117) limits lithium-ion transport and leads to high interfacial resistance and overpotential at the CEI.118,119 However, when applied as extremely thin nano-layers via atomic layer deposition (ALD), these limitations are reduced as the nanoscale thickness and grain boundaries facilitate lithium-ion migration.120 The surface of LFP was covered with a uniform Al2O3 nano-coating of about 5–6 nm without altering its bulk framework, as confirmed through X-ray photoelectron spectroscopy (XPS) analysis, and this stable coating remained intact even after 300 charge/discharge cycles, greatly improving capacity retention and rate capability at high cycling rates like 10C.36 Al2O3 coating does not vary the olivine framework of LFP, as all frameworks (pristine LFP/C, 1 LFP/C/Al2O3 and 2 LFP/C/Al2O3) shows pure phase with greater crystallinity.36
Using a chemical precipitation method, LFP/C composites were coated with MnO2, Al2O3 (ref. 109) and CuO, where XRD analysis confirmed that the olivine structure remained intact, and electrochemical tests showed substantial perfection in superior rate performance capability and cycling durability, among them, the MnO2-coated sample achieved a specific discharge capacity of 118.5 mAh g−1 at 3C with 93.7% capacity sustainability after 250 cycles, outperforming the uncoated material (95.1 mAh g−1).121
Graphitized CNTs were joined with an amorphous carbon coating to form a dual nano-carbon decorated LFP (LFP@C/CNT) nanocomposite. This is permissible for exceptional ultrafast charge/discharge performance (∼59% capacity retaining at 120 °C) and improved low-temperature capability (∼71.4% retaining at −25 °C).5,122 With an approximate crystallite size of about 90 nm on average, the orthorhombic LFP exhibits high phase purity, as shown by the XRD patterns in Fig. 17a. HRTEM (Fig. 17c–e) displays distinct lattice fringes, demonstrating the single-crystalline nature of LFP, whereas SEM images (Fig. 17b) show a uniform particle distribution. Each LFP particle is enclosed in a uniform 2–3 nm amorphous carbon layer, and connecting CNTs form a 3D conductive network (Fig. 17d) that improves electron transport. The FFT pattern (Fig. 17f) confirms the high crystallinity and orientation of the nanoparticles.5,122
Fig. 17. (a) XRD pattern, (b) SEM, (c and e) HRTEM images, (d) schematic illustration of the generated LFP@C/CNT nanocomposite, and (f) the corresponding FFT from the HRTEM in (e).122 Reproduced from ref. 122 with permission from John Wiley and Sons, copyright 2013.
6. Conclusions
LFP is a robust and stable cathode material for LIBs, celebrated for its intrinsic thermal robustness and outstanding cycling longevity. Unfortunately, slow lithium-ion diffusion, poor electronic/ionic conductivities and low bulk density limit its full potential. This review has systematically shed light on the evolution of LFP synthesis and modification strategies. Initially, efforts to overcome LFP's intrinsic limitations primarily revolved around carbon coating, which effectively improved electronic pathways. More recent advancements, however, highlight a significant paradigm shift towards sophisticated modification techniques. The incorporation of heteroatom doping, multi-walled carbon nanotubes (MWCNTs), and various metal oxide or nanoscale coatings has demonstrably enhanced both the electronic conductivity and rate capability of LFP cathodes. These modern approaches represent a crucial step forward, moving beyond traditional surface treatments to more intricate material engineering. The improvement in synthesis methods, emphasizing structural control and scalability, and post-synthesis modification techniques underscores a clear trajectory towards optimizing LFP. The enhanced performance achieved through these innovative strategies firmly positions LFP as a leading candidate for modern, highly efficient energy storage technologies, capable of meeting the escalating demands for efficient and sustainable battery technologies. The future research activities are expected to focus on synergistic approaches combining advanced synthesis with multi-component modification to unlock even greater electrochemical performance and durability in LFP cathodes. Furthermore, the incorporation of LFP with emerging solid-state electrolyte systems presents a particularly promising avenue toward the development of ASSLBs, which may offer improved safety, increased energy density, and enhanced long-term stability. These all advancements highlight the potential of LFP for the development of next-generation ASSLBs technologies.
Author contributions
Sania Ishtiaq: conceptualization, methodology, investigation,writing original draft preparation, visualization. Abdul Majid: supervision, validation, writing – review and editing, funding acquisition. Abdul Qadeer: investigation, resources, data curation. Mohammad Alkhedher: methodology, formal analysis, validation. Niyazi Bulut: conceptualization, project administration, writing review and editing.
Conflicts of interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Data availability
There is no additional data associated with this article.
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