Priyadarshi Roy
Chowdhury
a,
Himani
Medhi
b,
Krishna G.
Bhattacharyya
c and
Chaudhery Mustansar
Hussain
*d
aDepartment of Chemistry, Gauhati University, Guwahati-781014, Assam, India. E-mail: priyadarshiroychowdhury@outlook.com
bDepartment of Chemistry, Eastern Karbi Anglong College, Sarihajan-782480, Assam, India. E-mail: himanimedhi18@gmail.com
cDepartment of Chemistry, Assam Don Bosco University, Sonapur-782402, Assam, India. E-mail: kgbhattacharyya@gmail.com
dDepartment of Chemistry and Environmental Science, New Jersey Institute of Technology, Newark, NJ 07102, USA. E-mail: chaudhery.m.hussain@njit.edu
First published on 9th September 2025
Layered double hydroxides (LDHs) are emerging as critical materials for advancing the green hydrogen economy due to their versatility, cost-effectiveness, and tunable catalytic properties. Their layered structure allows for compositional flexibility, enabling optimization of active sites for efficient electron transfer. The objective of this review is to comprehend the latest advancements in the production of sustainable LDHs with a particular emphasis on their potential for the efficient electrochemical water splitting process involving both seawater and freshwater, which is essential for the generation of green hydrogen as a sustainable energy source. The strategies of green hydrogen generation and its mechanism have been critically discussed in this review. An overview is provided on the concept of green hydrogen economy involving LDH-based materials. Ongoing research into the design and application of LDHs is anticipated to provide a sustainable avenue for green hydrogen by integrating high catalytic efficiency, resource optimisation, and adaptability to practical conditions such as seawater electrolysis, thus realising their complete potential in decarbonising energy systems.
The concept of a green hydrogen economy revolves around the use of hydrogen as a clean energy carrier, produced primarily through the electrolysis of water using renewable energy sources. This approach aims to significantly reduce greenhouse gas emissions and dependence on fossil fuels, contributing to a more sustainable energy system. Green hydrogen is produced by electrolyzing water using electricity generated from renewable sources like solar, wind, or hydroelectric power.4 This process emits only water vapour and oxygen, making it a carbon-neutral energy source.5 The development of a green hydrogen economy offers a promising pathway to decarbonize hard-to-abate sectors, enhance energy security, and support sustainable development goals.
Layered double hydroxides (LDHs) are emerging as pivotal materials in advancing the green hydrogen economy due to their structural versatility, cost-effectiveness, and catalytic efficiency. Hydrotalcite, the naturally occurring prototype of LDH, was first identified in 1842. A hundred years later, in 1942, researchers succeeded in synthesizing the first LDHs, which also led to the establishment of the double-layer sheet concept in their preparation. LDHs have evolved from a mineral curiosity to a cornerstone of sustainable technology, with ongoing research focused on scalability, durability, and multifunctional applications in energy and environmental systems. Fig. 1 displays the timeline associated with the development of LDH materials. Its layered structure and tunable composition enhance active site exposure and electron transfer. Defects and vacancies in LDHs, such as those created by dissolving Mn+ ions, further could boost catalytic performance.6 LDHs and their derivatives (e.g., transition metal dichalcogenide composites) efficiently drive both oxygen evolution reaction (OER) and hydrogen evolution reaction (HER), enabling scalable electrolysis systems.7 LDHs derived from industrial waste also align with circular economy principles.8–10 The importance of this topic could be understood through the number of publications in ScienceDirect from 2021 to 2025 under the keyword ‘layered double hydroxides for green hydrogen generation’, depicted graphically in Fig. 2. LDHs could most likely address the challenges in seawater-based hydrogen production, since the hierarchical structures (e.g., hollow microspheres) of LDH-based materials have been reported to improve the surface area and stability, critical for industrial-scale brine electrolysis.8 Thus, LDHs bridge critical gaps in the green hydrogen value chain, from efficient water splitting to sustainable material sourcing, making them indispensable for achieving a carbon-neutral energy future. Innovations in their design and application would likely continue to drive down costs and improve performance, accelerating the transition to clean energy systems.11–23
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| Fig. 2 The number of articles available in ScienceDirect under the keyword ‘layered double hydroxides for green hydrogen generation’ from 2021–2025 (accessed on 17/03/2025; 00:52 IST). | ||
The objective of this review is to highlight the recent breakthroughs in LDH-based materials for sustainable hydrogen production, emphasizing their structural adaptability and versatility. The synthesis as well as functionalization strategies have also been mentioned in detail. The mechanistic pathways of these materials for HER, OER and overall water splitting (OWS) have been also been discussed in detail. Further, the review also emphasizes sustainable material design and waste utilization through the integration of a circular economy. It is anticipated that this review would bridge fundamental research and industrial applications by showcasing LDHs as versatile, scalable catalysts for green hydrogen production. Furthermore, this review also emphasizes the role of LDHs in reducing carbon footprints, enhancing energy efficiency, and aligning with global sustainability goals.
The hydrothermal process also results in crystallite size optimization. For ZnCr-LDH, the catalytic activity was found to increase steadily with crystallite size (up to about 18 nm), which was attributed to enhanced charge-carrier separation.14 The hydrothermal synthesis process also has been reported to engineer morphologically the LDH structures. A separate study reported that Ni/Al-LDH nanorods synthesized at 180 °C exhibit enhanced surface area and stability, ideal for sustained catalytic activity.3 Hydrothermal synthesis also follows green synthesis considerations involving waste utilization.23 Hydrothermal methods have been reported to incorporate industrial byproducts while maintaining low energy inputs (e.g., hydrocalumite synthesis from Ca/Al-rich waste). Hydrothermal processes also follow reduced chemical footprint (e.g., HMT as a single precipitant) and align with sustainable production goals.14,22 The comparative results of hydrogen production with some hydrothermally synthesized LDHs and LDH-based composites have been presented in Table 1. The schematic illustration of the different stages of hydrothermal synthesis of LDHs from waste precursors, involving the various stages of its formation, viz., nucleation, growth, crystallization and aggregation leading to electrochemical water splitting, thereby generating green hydrogen and oxygen is presented in Fig. 3. The recent advancements highlight hydrothermal synthesis as a versatile route for tailoring LDH properties, with ongoing research focusing on scaling production and integrating machine learning for parameter optimization.
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| Fig. 3 Schematic representation of the various phases of hydrothermal synthesis of LDHs for green hydrogen production (Adapted with permission from ref. 24©2025, Royal Society of Chemistry and ref. 25©2024, Elsevier). | ||
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| Fig. 4 Schematic depicting a green solvent-free NiFe-LDH for efficient OER and HER (reproduced with permission from ref. 26©2024, The American Chemical Society). | ||
The study reported the synergistic consequences via the creation of large electrochemically active sites with well-connected metal ions having nano-spherical architectures. The study also reported that higher OER and HER efficiency could be achieved by optimising the appropriate stoichiometric ratio viz, Ni6Fe4LDH. According to the linear sweep voltammetric (LSV) curves [Fig. 5(a)], the LDH at the Ni6Fe4LDH stoichiometric ratio showed increased OER activity at a current density (10 mA cm−2) in 1 M KOH, with an overpotential of 280 mV [Fig. 5(c)] and a reduced Tafel slope of 116 mV dec−1 [Fig. 5(b)], as compared to other electrocatalysts like IrO2, Ni(OH)2, Fe(OH)2, and NF. Meanwhile, polarisation curves corresponding to HER that were measured between the potential range of −0.4 and 0.0 V were used to assess the HER behaviour of LDH/NF. The Ni6Fe4 LDH electrode depicted higher catalytic activity than other catalysts, according to the LSV curves shown in Fig. 6(a). Again, with overpotentials of 167 mV [Fig. 6(c)] (at a lower Tafel slope of 112 mV dec−1) [Fig. 6(b)] for the HER, the ideal Ni6Fe4LDH ratio achieved 10 mA cm−2 (current density) in 1 M KOH. Furthermore, Ni6Fe4LDH exhibited remarkable resilience, remaining steady for 90 hours with a slight drop in current density of 4.1 [Fig. 6(d)] and 4.6% [Fig. 5(d)] for the HER and OER, respectively.26 Interestingly, efficient water electrolysis was achieved in the bifunctional two-electrode configuration of Ni6Fe4LDH/NF‖Ni6Fe4LDH/NF, maintaining a steady current density (= 10 mA cm−2) at a bias of 1.64 V for more than 140 h, with a minor current loss of 3.9% of the current density.
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| Fig. 5 OER (a) LSV curves (b) Tafel plot (c) overpotentials (at 10 mA cm−2) of Ni6Fe4LDH/NF, IrO2/NF, Ni(OH)2/NF, Fe(OH)2/NF and bare NF (d) current density vs. time plot for Ni6Fe4LDH/NF (reproduced with permission from ref. 26©2024, The American Chemical Society). | ||
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| Fig. 6 HER (a) LSV curves (b) Tafel plot (c) overpotentials (at 10 mA cm−2) of Ni6Fe4LDH/NF, Pt/C/NF, Ni(OH)2/NF, Fe(OH)2/NF and bare NF (d) current density vs. time plot for Ni6Fe4LDH/NF (reproduced with permission from ref. 26©2024, The American Chemical Society). | ||
| Waste-derived LDHs | Waste sources | Stability; electrolyte | η j (mV) @ j = 10 mA cm−2 | Tafel slope (mV dec−1) | Ref. | ||
|---|---|---|---|---|---|---|---|
| OER | HER | OER | HER | ||||
| η j : overpotential and current density j (= 10 mA cm−2). | |||||||
| Ni0.5Mn0.3Co0.2(OH)2 | Li-ion battery | 24 h; 1 M KOH | 280 | — | 6.79 | — | 28 |
| De-lithiated Li0.4Ni0.5Co0.2Mn0.3O2 | 80 h; 1 M KOH | 236 (η20) | — | 66 | — | 29 | |
| NiFe-LDH/Cu(OH)2/Cu | Cu-cable wire | 24 h @ 20 mA cm−2; 1 M KOH | 275 (η20) | — | 83 | — | 30 |
| 390 (η100) | |||||||
| NiFe-borate LDH/N-doped carbon | C and N-doped C procured from Mangosteen skin | 24 h; 1 M KOH | 243 | — | 42.7 | — | 31 |
| NiFe-borate LDH | —; 1 M KOH | 255 | — | — | — | ||
| NiFe-C LDH | —; 1 M KOH | 274 | — | — | — | ||
| NiFe LDH/(NiFe)Sx/CMT(NiFe)Sx/CMT | CMT procured from Willow catkins | 15 h @ 10 mA cm−2 | 210 | 169 | 31 | 120 | 32 |
| — | 300 | 266 | — | — | |||
| NiCaFe-LDH | Bio-waste derived from egg-shell | 8 h @ 1.5 mA cm−2 and 1.65 V; 0.1 M PO43− buffer at pH 7 | 373 | — | 13 | — | 33 |
Again, the performance of several recently reported waste-derived LDH-based electrocatalysts with their key features, for OER, HER, and OWS under alkaline and high current density (HCD) conditions have been depicted in Table 3.
| Electrocatalyst | Reaction | Waste sources | Conditions | Performance metrics | Key features |
|---|---|---|---|---|---|
| NiFe-LDH derived from red mud | OER | Red mud (industrial waste) | 1 M KOH | Overpotential: ∼300 mV @ 10 mA cm−2 | High Fe3+ content enhances active sites; require conductivity enhancement.34,35 |
| MgAlFe-LDH from steel slag | HER | Steel slag | 1 M KOH | Overpotential: ∼250 mV @ 10 mA cm−2 | Effective Fe3+/Al3+ utilization; moderate HER performance.34,36 |
| NiCo-LDH from mining residues | OWS | Mining residues | Alkaline medium | Overall voltage: 1.58 V @ 10 mA cm−2 | Bifunctional activity; improved conductivity via Co doping.35,37 |
| Ochre-derived LDH | OER | Ochre waste | 0.1 M KOH | Overpotential: ∼310 mV @ 10 mA cm−2 | Defect engineering improves catalytic activity |
| NiFe-LDH@biochar composite | OWS | Biomass ash | Alkaline medium | Overall voltage: 1.55 V @ 10 mA cm−2 | Biochar improves conductivity and stability.34,36 |
| ZnCo-LDH from e-waste | HER/OER | Electronic waste | 1 M KOH, HCD | HER overpotential: ∼220 mV @ 100 mA cm−2 OER overpotential: ∼280 mV @ 100 mA cm−2 | High durability under HCD; Zn-Co synergy enhances performance.35,37 |
| CoCuFe-LDH/graphene | Metal waste | OER/HER | Alkaline | OER onset potential: 1.52 V; HER onset potential: −0.32 V; Tafel slope: 62.8–76.6 mV dec−1 | Graphene enhances conductivity; optimized via factorial design for HCD stability.38 |
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| Fig. 7 (a) Schematic representation of the relative band position and charge transfer phenomenon of MgCr-LDH nanoparticles for the photoelectrochemical water splitting. (b) Plot of current density over applied potential (vs. RHE) for pristine MgCr-LDH/NS and MgCr-LDH/PS nanoparticles under light and dark. (c) Plot depicting the comparative study of current density over applied potential (vs. RHE) for MgCr-LDH/NP under light and dark. (d) Comparative Tafel plots of the pristine LDH over nanoparticles and nanosheets (adapted with permission from ref. 39©2022, Springer Nature; License: CC-BY 4.0). | ||
Fig. 7(b) and (c) presents the plot of current density vs. applied potential under light and dark conditions. The material depicted efficient photoelectrochemical properties with a low Tafel slope of 82 mV decade−1 and a current density of 6.9 mA cm−2. The comparative Tafel slope of the pristine LDH over nanoparticles and nanosheets could be evident from Fig. 7(d). The study also reported that under visible light, MgCr-LDH nanoparticles presented photocatalytic H2 evolution of 1315 μmol h−1; which was 1.8 and 4.3 times higher than that of MgCr-LDH nanosheets (726 μmol h−1) and pristine MgCr-LDH (300 μmol h−1), respectively.39
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| Fig. 8 (a)–(e) Schematic representation of the important strategies for chemical component adjustment in LDHs (adapted with permission from ref. 47©2023, Elsevier). | ||
| Chemical component adjustment | HER activity | OER activity | Current density (mA cm−2) | Overpotential (mV) | Tafel slope (mV dec−1) | Stability |
|---|---|---|---|---|---|---|
| CoCuFe-LDH/graphene41 | Onset voltage: −0.32 V (HER) | Onset voltage: 1.52 V (OER) | 10–100 | HER: ∼220 (100 mA cm−2) OER: ∼280 (100 mA cm−2) | HER: 76.6 OER: 62.8 | >24 h @ 10 mA cm−2 (90% retention) |
| NiFeMn-LDH42 | — | 270 mV @ 10 mA cm−2 | 10 | 270 | 76 | >10 h @ 50 mA cm−2 |
| NiFe-LDH/Ni Foam43 | — | 223 mV @ 10 mA cm−2 | 10 | 223 | 48.9 | >24 h @ 10 mA cm−2 |
| NiFeV-LDH44 | — | 210 mV @ 10 mA cm−2 | 10 | 210 | 39 | >50 h @ 10 mA cm−2 |
| Pt-NiFe-LDH45 | 120 mV @ 10 mA cm−2 | 204 mV @ 10 mA cm−2 | 10 | HER: 120 OER: 204 | HER: 68 OER: 56 | >50 h @ 10 mA cm−2 |
| NiLa-LDH44 | — | 209 mV @ 10 mA cm−2 | 10 | 209 | 42 | — |
| NiFe-LDH@Biochar46 | — | — | 10 | OWS voltage: 1.55–1.58 V | — | — |
Moreover, doping and electronic modulation has resulted in the synthesis of V-doped NiFe LDH. In this study, V has been introduced into NiFe-LDH by forming an electron transport chain (Ni–O–Fe–O–V–O–Ni), optimizing binding with reaction intermediates and accelerating electron transfer.49 This dual strategy (heterostructure + doping) reduced OER overpotential to 280 mV at 100 mA cm−2. A comparative study of HER, OER, and OWS based on heterojunction-constructed LDH-based electrocatalysts is presented in Table 5.
| Heterojunction construction strategy | HER activity | OER activity | Current density (mA cm−2) | Overpotential (mV) | Tafel slope (mV dec−1) | Stability |
|---|---|---|---|---|---|---|
| Co(OH)F@CoFe-LDH (core–shell nanorods)52 | Overpotential: 130 @ 10 mA cm−2 | Overpotential: 240 @ 10 mA cm−2 | 10 | OWS voltage: 1.58 V | — | 37 h @ 10 mA cm−2 |
| Ni3S2@V-NiFe(III)LDH (doped heterostructure)53 | — | Overpotential: 280 @ 100 mA cm−2 | 100 | 280 | 45.4 (OER) | — |
| CoMn-LDH (self-assembled hierarchical)54 | Overpotential: −199 @ 10 mA cm−2 | Overpotential: 340 @ 10 mA cm−2 | 10 | — | 102 (OER), 128 (HER) | 63% retention after 20k cycles |
| CoMn@CuZnFeS (ternary composite)54 | Overpotential: −222 @ 10 mA cm−2 | Overpotential: 366 @ 10 mA cm−2 | 10 | — | 160 (HER) | — |
| NiFeMn-LDH/OOH-graphene (heterojunction +conductive support)55 | — | Overpotential: 338 @ 10 mA cm−2 | 10 | — | 67 (OER) | — |
| Nanostructure engineering strategy | HER activity | OER activity | Current density (mA cm−2) | Overpotential (mV) | Tafel slope (mV dec−1) | Stability |
|---|---|---|---|---|---|---|
| Pt-NiFe-LDH/CC (sub-nano Pt clusters)56 | Overpotential: 120 mV @ 10 mA cm−2 | Overpotential: 204 mV @ 10 mA cm−2 | 10 | HER: 120 OER: 204 | HER: 68 OER: 56 | Stable for >50 h under alkaline conditions |
| CoMn-LDH nanosheets57 | Overpotential: −199 mV @ 10 mA cm−2 | Overpotential: 340 mV @ 10 mA cm−2 | 10 | HER: −199 OER: 340 | HER: 128 OER: 102 | Retains 63% capacitance after 20 000 cycles |
| NiFe-LDH/Ni Foam (nanosheet array)58 | — | Overpotential: 223 mV @ 10 mA cm−2 | 10 | OER: 223 | OER: 48.9 | Stable for >24 h @ 10 mA cm−2 |
| Gd-Doped NiFe-LDH nanosheets56 | — | Enhanced OER activity via oxygen vacancies and porous morphology | 10 | ∼250 | — | Stable under alkaline medium |
| Ni3S2@V-NiFe(III) LDH heterostructure59 | — | Overpotential: 280 mV @ 100 mA cm−2 | 100 | OER: 280 | OER: 45.4 | — |
| MgAl-LDH via exfoliation60 | — | Moderate OER activity | 10 | ∼300 | — | Stable colloidal suspension |
A study reported the generation of self-supported PtQDs@NiFe-LDH through a two-step facile approach involving chemical etching.61 The synthesis strategy has been schematically presented in Fig. 9(A). The SEM and TEM images of the QD-LDH hybrid presented an orderly arrangement of LDH nanosheets on NF [Fig. 9(B) and (C)]. The XRD of the QD-LDH represented the characteristic peaks showing the doping of QDs into the corresponding NiFe LDH (JCPDS card no. 40-0215). Apart from the characteristic LDH peaks, the XRD peaks at 39.7°, 46.2°, and 67.4° could be attributed to the corresponding peaks (111), (200), and (220) due to the successful doping of PtQDs onto the LDH (following JCPDS card no. 40-0215) [Fig. 9(D)]. The interplanar spacing was reported to be 0.225 nm, corresponding to (015) plane of NiFe LDH (015) plane of NiFe LDH [Fig. 9(F)]. The dispersion of PtQDs on the LDH nanosheets could be evident from the spots marked in pink circles in Fig. 9(E) and (F). The average diameter of PtQDs in PtQDs@NiFe LDH was reported to be approximately 2.2 nm [Fig. 9(G)]. The EDX mapping revealed the existence of Ni, Fe, O, and Pt in the PtQDs@NiFe LDH [Fig. 9(H)–(L)]. The loading of Pt by mass has most likely contributed to the abundance of active sites for the HER process.
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| Fig. 9 (A) Schematic illustration of the synthesis of PtQDs@NiFe LDH, (B) and (C) SEM and HR-TEM images of PtQDs@NiFe LDH; (D) XRD pattern of PtQDs@NiFe LDH and NiFe LDH; (E) and (F) HRTEM images of PtQDs@NiFe LDH; (G) average particle size distribution of PtQDs; (H)–(L) EDX mapping patterns of various elements within PtQDs@NiFe LDH (reproduced with permission from ref. 61©OAE publishing, Inc.; License: CC-BY 4.0). | ||
The HER performance was evaluated at 1 M KOH solution. It was reported that PtQDs@NiFe LDH exhibited superior HER performance compared to NiFe LDH, Pt/C, and NF [Fig. 10(A) and (B)]. The intrinsic activity [Fig. 10(C)] revealed that PtQDs@NiFe LDH possessed highest j0 (= 4.325 mA cm−2), as compared to the control samples, indicating excellent HER efficiency. The plot of Δη/Δlog|j| for PtQDs@NiFe LDH vs. current density presented a high current density for PtQDs@NiFe LDH, representing its superior HER efficiency as compared to other catalysts [Fig. 10(D)]. Meanwhile, Fig. 10(E) revealed that PtQDs@NiFe LDH exhibited the smallest semicircle diameter (= 1.62 Ω), in comparison to other catalysts, depicting its high kinetics associated with charge transfer. Additionally, PtQDs@NiFe LDH exhibited a double-layer capacitance (Cdl) of 55 mF cm−2, which is higher than that of the other control samples observed in this study [Fig. 10(E)]. Fig. 10(G) revealed a higher current density of the PtQDs@NiFe LDH, in comparison to other catalysts. Fig. 10(H) represents the lowest Tafel slope, as compared to other catalysts, indicating its higher HER efficiency. Thus, the results indicate that PtQDs@NiFe LDH possess superior HER efficiency, highlighting their remarkable potential for industrial purposes.
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| Fig. 10 HER curves (A) LSV plots; (B) plot of overpotential vs. log (current density); (C) j0 of PtQDs@NiFe LDH some control samples are derived by Tafel plots; (D) Plot of Δη/Δlog|j| versus current density ranges; (E) comparative Nyquist plots; (F) plot of current density vs. scan rate; (G) potential vs. time plots (H) plot of Tafel value vs. overpotential of PtQDs@NiFe LDH over other catalysts (reproduced with permission from ref. 61©OAE publishing, Inc.; License: CC-BY 4.0). | ||
The study also presented the OWS efficiency of the electrocatalysts to expedite their potential for industrial applications. Since, OER is a vital component of OWS, the OER activity of PtQDs@NiFe LDH-1, PtQDs@NiFe LDH, PtQDs@NiFe LDH-5 electrocatalysts, and NiFe LDH precursor was evaluated. Fig. 11(A) and (B) presented highly efficient OER of NiFe LDH over other PtQDs loaded samples due to the exceptionally low overpotential of NiFe LDH over other samples. Moreover, a two-electrode system was constructed involving PtQDs@NiFe LDH, having high HER (as cathode) and NiFe LDH having highly efficient OER (as anode), represented by PtQDs@NiFe LDH (−)‖NiFe LDH (+), for evaluation of OWS efficiency. Separate two-electrode systems were assembled and as Pt/C (−)‖RuO2 (+) for comparative study.
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| Fig. 11 OWS results; (A) LSV plots; (B) plot depicting comparison of overpotentials at different current densities; (C) potential vs. current density plots PtQDs@NiFe LDH (−)‖NiFe LDH (+) and Pt/C (−)‖RuO2; (D) plot of potential (cell voltage) vs. current density (E) potential vs. time plot depicting stability in OWS process; (F) snapshots representing the OWS experimental set up and extent of gas collection at different instances; (G) plot depicting measured volume of H2 or O2 against theoretically produced H2 or O2 w.r.t. time; (H) potential comparison of PtQDs@NiFe LDH (−)‖NiFe LDH (+) over other reported electrocatalysts (reproduced with permission from ref. 61©OAE publishing, Inc.; License: CC-BY 4.0). | ||
Fig. 11(C) and (D) exhibited superior OWS efficiency with high current density of PtQDs@NiFe LDH (−)‖NiFe LDH (+) electrode system over Pt/C (−)‖RuO2 (+). PtQDs@NiFe LDH (−)‖NiFe LDH (+) electrolyzer only needed 1.54, 1.75, and 2.02 V of applied voltages to achieve 100, 1000, and 2000 mA cm−2, respectively, which is much higher than that observed for Pt/C (−)‖RuO2 (+) systems, thereby depicting highly efficient OWS process with PtQDs@NiFe LDH (−)‖NiFe LDH (+). The electrode system, PtQDs@NiFe LDH (−)‖NiFe LDH (+), also presented high stability at 100 mA cm−2 for 200 h [Fig. 11(E)]. Fig. 11(F) presented the snapshots representing the OWS experimental set-up of PtQDs@NiFe LDH (−)‖NiFe LDH (+) system and the extent of gas collection at different instances. Fig. 11(G) highlighted the plot depicting measured volume of H2 or O2 against the theoretically produced H2 or O2 w.r.t. time. It was reported that the ratio of H2
:
O2 in OWS = 2
:
1, representing the Faraday efficiency (FE) ∼ 100%, depicting an excellent OWS catalytic activity with PtQDs@NiFe LDH (−)‖NiFe LDH (+) systems over other reported electrocatalysts. The encouraging OWS results [Fig. 11(H)] highlight the significant potential of PtQDs@NiFe LDH (−)‖NiFe LDH (+) electrolyzing systems for industrial uses over other commercial catalytic systems. Moreover, Table 7 summarizes several quantum dot modified and doping strategies for LDH-based materials and their impact on the HER, OER, and stability of LDH-based electrocatalysts.
| Quantum dot modification strategy | HER activity | OER activity | Current density (mA cm−2) | Overpotential (mV) | Tafel slope (mV dec−1) | Stability |
|---|---|---|---|---|---|---|
| Pt QDs@NiFe LDH61–63 | Overpotential: 92 mV @ 500 mA cm−2, 252 mV @ 2000 mA cm−2 | OWS voltage: 1.66 V @ 500 mA cm−2, 2.02 V @ 2000 mA cm−2 | 500–2000 | HER: 92–252 OWS: 1.66–2.02 V | HER: 35 | Stable for >200 h under industrial conditions |
| CdMoSe-QD/NiV-LDH (S-scheme heterojunction)64 | Photocatalytic H2 production rate: 7.36% ACE | Photocatalytic H2O2 production rate: 1.67% SCC | — | — | — | Enhanced photocatalytic stability due to delayed recombination of excitons |
| Pt QDs@S-NiFe LDH (Sulfur-doped)62,63 | Overpotential: 53 mV @ 100 mA cm−2, 140 mV @ 1000 mA cm−2, 252 mV @ 2000 mA cm−2 | OWS voltage: 1.54 V @ 100 mA cm−2, 1.75 V @ 1000 mA cm−2 | 100–2000 | HER: 53–252 OWS voltage: 1.54–1.75 V | HER: ∼40 | Stable for >55 h at high current densities |
| Carbon QD/NiFe-LDH Composite65 | — | Overpotential: ∼300 mV @ moderate current densities | Moderate | ∼300 | — | Stable under alkaline conditions |
| ZnS QDs-ZnAl-LDH64,66 | Solar water splitting efficiency | Photocatalytic hydrogen evolution | — | — | — | Enhanced photocatalytic durability due to quantum confinement effect |
Inspite of these shortcomings, LDHs are among the best alkaline OER catalysts as it could self-reconstruct into active oxyhydroxide phases and have high intrinsic activity. In order to overcome these limitations, practical mitigation strategies should include using bipolar membranes (BPM) or three-compartment designs with LDHs so the anolyte is alkaline and chloride could be excluded from the anode compartment, substantially reducing CER risk.68 Another, strategy could be using a central saline compartment with selective ion traps or a buffer layer for reducing direct Cl− flux to the anode.69–71 Moreover, LDH surface/interlayer engineering (doping, phosphate intercalation, protective shells) along with operational pretreatment could manage scaling.
On the other hand, a comparative cost perspective on “green” synthesis of LDHs for OER reveals that conventional hydrothermal methods, though widely employed, are resource-intensive owing to their reliance on high-temperature (120–200 °C) and high-pressure conditions, long reaction durations, and the use of significant volumes of solvents, all of which raise both capital and operational expenditure. In contrast, solvent-free approaches such as mechanochemical grinding, solid-state reactions, and molten-salt methods have been significantly reducing synthesis costs by eliminating solvent purchase and recovery, shortening reaction times, and minimizing energy demand. These strategies could not only lower the overall energy footprint but also decrease environmental management costs associated with solvent disposal, aligning with the principles of green chemistry. Nonetheless, challenges remain regarding large-scale morphology control and reproducibility, which hydrothermal systems currently address more effectively. Therefore, while solvent-free methods are economically and environmentally advantageous for sustainable LDH production, further optimization is needed to achieve industrial scalability. Continued innovation in their design and hybridization is expected to further unlock their potential for sustainable hydrogen production. A comparative table (Table 8) of recently reported LDH-based electrocatalysts for HER, OER and OWS involving seawater under natural alkaline, artificial alkaline and artificial alkaline with added NaCl is listed herein.
| Electrocatalyst | Conditions | Reaction | Current density (mA cm−2) | Overpotential (mV) | Tafel dlope (mV dec−1) | Stability |
|---|---|---|---|---|---|---|
| MgAlCe-LDH/β-Ni(OH)2/Ni foam72 | Natural seawater (alkaline) | OER | 10 | 80 | — | 25 h @ 15 mA cm−2 |
| HER | 10 | 337 | — | |||
| OWS | 10 | 1.42 V (cell voltage) | — | |||
| ZnFe LDH@NiCoS/NF73 | Alkaline seawater (1 M KOH + seawater) | OER | 10 | 284.8 | 81.5 | 50 h @ 10 mA cm−2 |
| HER | 10 | 246.3 | 74.6 | |||
| OWS | 10 | 1.593 V (cell voltage) | — | |||
| NiFe-LDH74 | Artificial alkaline seawater (KOH + 0.5 M NaCl) | OWS | 600 (HCD) | — | — | 100 h @ 600 mA cm−2 |
A comprehensive comparison of LDH-based materials for alkaline seawater and freshwater splitting, based on recent studies, has been presented in Table 9. Alkaline conditions suppress chlorine evolution (Cl− → ClO−/ClO3−) by widening the potential gap between OER and the chlorine evolution reaction (CER).
| Catalyst | Electrolyte | Overpotential (mV) @ 10 mA cm−2 | Cell voltage (V) @ 10 mA cm−2 | Stability | Key features |
|---|---|---|---|---|---|
| Se-FeCo-LDH75 | Alkaline seawater | OER: 229 @ 100 mA cm−2 | 1.491 | 245 h @ 10 mA cm−2 | Partial selenization forms an anion barrier to repel Cl−, improving durability. |
| NiCo-LDH-OH76 | Freshwater (1 M KOH) | HER: 180 OER: 317 | — | 20 h @ 10 mA cm−2 | Alkali treatment creates metal vacancies, improving HER/OER activity. |
| Ru/Fe-NiCr-LDH77 | Freshwater (alkaline) | — | 1.6–2.0 V @ 262.5 mA cm−2 | Scalable AEM WE system | Ru/Fe doping optimized electronic structure for efficient H* and OOH* steps. |
A comparative analysis of recently reported LDH-based electrocatalysts for OWS and OER involving alkaline freshwater, simulated seawater, alkaline seawater, alkaline industrial sewage water has been summarized in Table 10.
| Catalyst | Conditions | Reaction | Current density (mA cm−2) | Overpotential (mV) | Tafel slope (mV dec−1) | Stability |
|---|---|---|---|---|---|---|
| NiFeCrCo LDH78 | Alkaline freshwater (1 M KOH) | OWS | 10/100 | Overall voltage = 1.42 V/1.54 V | — | >120 h (simulated seawater) |
| Simulated seawater (1 M KOH + NaCl) | OWS | 10/100 | Overall voltage = 1.57 V/1.71 V | — | >120 h | |
| NiCo@NiFe LDH79 | Alkaline seawater (1 M KOH + seawater) | OER | 100/500 | 222/266 | 46.1 (OER) | >100 h @ 500 mA cm−2 |
| NiCoFe-LDH80 | Alkaline industrial sewage (6 M KOH) | OER | 10/500 | 274 @ 10 1.68 V @ 500 | — | Stable at industrial currents |
| FeOOH/CoFe LDH81 | Simulated seawater (1 M KOH + 0.5 M NaCl) | OER | 100/400 | 320 @ 400 (25 °C) 257 @ 400 (60 °C) | — | 300 h @ 100 mA cm−2 |
| NiTe@NiFe-LDH82 | Alkaline seawater (1 M KOH + seawater) | OER | 100/500 | 277/359 | 68.66 (OER) | 50 h @ 100 mA cm−2 |
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| Fig. 12 Mechanistic pathways of OER involving LDH-based materials in alkaline conditions, (a) AEM, (b) IMOC, (c) LOM. Various states involved in the reaction pathways have been designated by Sn and O–O coupling is depicted by dashed lines and highlighted (in Gray). The transition state (TS) of the coupling step is presented in the middle of each cyclic route (d) identification of different reaction models involved in AEM, IMOC and LOM, respectively, in the case of OER with LDH-based materials (reproduced with permission from ref. 83©2025, Springer Nature; License-CC-BY-4.0). | ||
The IMOC route associated with Ni(M)OOH [Fig. 12(b)] has been reported to proceed through the aggregation of the adsorbates lying in the vicinity to generate O–O coupling, leading to the formation of two branches. In branch (a) O–O coupling occur between two neighbouring *OH (S1), while in branch (b), associated with step S2, O˙* is formed at first, followed by the generation of O–O bond and subsequently –OOH respectively.
The LOM has been reported to exhibit contrasting route in comparison to the AEM and IMOC, coupling the Olatt bridging with the vicinity adsorbate to generate O–O coupling [Fig. 12(c)]. There are also two branches in LOM process. In branch (a), Olatt has been reported to couple with *OH in S1 step, while in branch (b) Olatt reportedly coupled to O˙* after S2 is generated. The utilized Olatt is subsequently recovered by electro-oxidation and OH− deprotonation.
The LOM directly engages oxygen atoms from the LDH lattice, thereby bypassing the conventional scaling relationship between *O and *OOH intermediates. This often results in reduced overpotentials and improved catalytic performance. For LOM to proceed effectively, the LDH lattice framework must enable reversible oxygen extraction and replenishment while preserving structural integrity.83
LDHs consist of positively charged brucite-like sheets, where divalent and trivalent metal cations are coordinated to hydroxyl groups.22,23,83 These layers are interspaced with charge-balancing anions and water molecules, endowing the material with intrinsic structural flexibility. Such a configuration renders LDHs more “breathable” compared to rigid oxide frameworks like rutile or perovskite.
The flexibility of the LDH lattice is central to promoting LOM. Dynamic metal–oxygen coordination allows local distortion of M–O octahedra during redox cycling, which in turn supports the formation and recombination of oxygen vacancies. This structural adaptability enables lattice oxygen to actively participate in the oxygen evolution reaction (OER).
Additionally, the layered structure could accommodate non-stoichiometry, as interlayer anions and hydroxide sheets mitigate the strain associated with oxygen extraction, thus preventing structural collapse and facilitating reversible lattice oxygen participation.
Moreover, lattice flexibility enhances metal-oxygen covalency, in transition metal based LDHs, by improving orbital overlap between O 2p and metal 3d states. This electronic feature strongly favours lattice oxygen redox processes. LDHs could also undergo localized strain relaxation, such as expansion or compression around catalytic sites, thereby lowering the energy barrier for oxygen release and accelerating LOM pathways.83
Finally, the interlayer constituents play a vital role in structural recovery. After lattice oxygen involvement in OER, intercalated anions (e.g., OH−, CO32−) and water molecules assist in re-oxidizing the framework, ensuring sustained catalytic activity. Collectively, these structural and electronic attributes make LDHs particularly well-suited as efficient and durable catalysts operating via the lattice oxygen mechanism.
The study further reported that the O–O coupling steps in AEM process follow the Eley–Rideal (ER) model and involve adsorbed O˙* reacting with a H2O molecule in the electrolyte [Fig. 12(d)]. The O–O coupling steps in the IMOC process have been reported to follow the Langmuir–Hinshelwood (LH) model, involving the adsorbed reactants only. The Olatt of the catalyst is consumed O–O coupling in the Mars–van Krevelen (MvK) model, being followed by the LOM pathway during the OER process.
LDHs are emerging as highly effective and tunable electrocatalysts for HER, especially in alkaline media. Their unique structure, compositional flexibility, and ability to host multiple active sites make them attractive for sustainable hydrogen production.84–86 The fundamental HER pathways in alkaline solution proceed through two main steps. The first step is regarded as Volmer step, in which water molecule adsorption and dissociation on metal sites occur, producing adsorbed hydrogen (H*) and hydroxide (OH−).
| H2O + e− → H* + OH− | (1) |
| H* + H2O + e− → H2 + OH− | (2) |
| 2H* → H2 | (3) |
LDHs are among the most promising earth-abundant electrocatalysts for OWS, efficiently catalyzing both the HER and OER in alkaline media. Their unique layered structure, tunable composition, and ability to host multiple active sites underpin their high performance and versatility. OWS consists of two half-reactions:
HER (at cathode)
| 2H2O + 2e− → H2 + 2OH− | (4) |
OER (at anode)
| 4OH− → 2H2O + O2 + 4e− | (5) |
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| Fig. 13 Schematic representation of the concept of a green hydrogen ecosystem with LDH-based materials. | ||
A study reported that NiFe-LDH hollow microspheres synthesized via a SiO2-templated method achieved an ultra-low OER onset overpotential of 239 mV at 10 mA cm−2, outperforming commercial Ir/C catalysts. The hierarchical structure has been reported to enhance active site exposure and ion transport, yielding a current density of 71.69 mA cm−2 at 300 mV overpotential and stability over prolonged operation.87 A separate study also reported that exfoliated CoAl-LDH nanosheets with oxygen vacancies reduced the coordination numbers (Co–O from 4.2 to 3.7) and enhanced conductivity, enabling stable OER performance for 110 hours.88 A separate study also reported the integration of LDHs with transition metal dichalcogenides (TMDs, e.g., MoS2) enhanced the HER/OER synergy due to tunable metal centers, exposed edge sites and layered structure. LDH-TMD together could enable efficient overall water splitting, particularly in seawater electrolysis, by mitigating corrosion and improving kinetics.89
Sustainable production of LDHs could be achieved via waste utilization, since LDHs derived from industrial waste align with circular economy principles. A study reported that NiFe-LDHs synthesized from industrial byproducts retain high catalytic activity, with Ni extraction enabling heterostructures like Ni2P@NiFe hydroxide. These systems have been reported to achieve 1.51 V cell voltage for overall water splitting while addressing hazardous waste challenges.90,91 Energy-efficient synthesis (e.g., hydrothermal/electrochemical methods) also minimises toxic byproducts. For example, microwave-assisted techniques have been reported to produce bifunctional NiCo2P catalysts90 with 1.44 V cell voltage at 10 mA cm−2. A separate study reported that Pd-loaded ZnTiAl-LDOs derived from LDH precursors, could produce hydrogen from glucose at 1.328 mmol g−1 h−1, outperforming Ni/Mg-based systems. Enhanced surface area (204 m2 g−1) and optimized band gaps have been reported to drive biomass conversion efficiency.92 The LDOs have been reported to undergo photocatalytic reforming to enable sustainable hydrogen generation from biomass waste, aligning with renewable energy integration.
LDHs have been documented to mitigate corrosion and stability issues in seawater-based electrolysis. A recent study demonstrated that CoFeAl-layered double hydroxides (CoFeAl-LDHs) exhibit remarkable corrosion resistance during seawater electrolysis, crucial for sustainable hydrogen production. During operation at high current densities (2 A cm−2) in concentrated seawater, Al3+ ions in the LDH are gradually etched by OH−, leading to the formation of Al(OH)4− species. This self-generated Al(OH)4− layer adsorb onto the electrode surface, acting as a protective barrier against chloride-induced corrosion. As a result, the CoFeAl-LDH anode maintained stable performance for over 350 hours, with minimal decay in OER activity, even under severe brine conditions. This self-protection mechanism not only enhanced electrode longevity but also bridged critical gaps in the green hydrogen value chain. LDHs like CoFeAl-LDHs combine efficient catalysis, corrosion resistance, and the potential for sustainable material sourcing, making them indispensable for scalable, carbon-neutral hydrogen production through seawater electrolysis.93,94 Continued innovation in defect engineering, waste valorization, and structural design will accelerate their adoption in global clean energy systems.
While LDHs have shown promise in laboratory settings, further improvements in long-term stability and resistance to degradation (especially under industrial current densities and in seawater) are needed to meet commercial requirements. Continued research into the identification of active sites, reaction intermediates, and degradation pathways using advanced in situ and operando techniques will be crucial for optimizing LDH performance and durability.
The development of environmentally benign, cost-effective, and scalable synthesis methods (such as one-step processes using abundant minerals) will also facilitate the widespread adoption of LDHs in hydrogen production technologies. Moreover, LDH-based catalysts are well-suited for coupling with intermittent renewable energy sources, and their further optimization could accelerate the deployment of decentralized, sustainable hydrogen production systems.
Thus, LDHs bridge critical gaps in the green hydrogen value chain, from efficient, earth-abundant catalysis to sustainable material sourcing and robust performance in diverse environments. Continued innovation in their design, synthesis, and mechanistic understanding will be pivotal for realizing scalable, carbon-neutral hydrogen production in both freshwater and seawater contexts.
P. R. C. and H. M. contributed towards conceptualization, literature research, visualization and writing the original draft. K. G. B. and C. M. H. contributed towards review, editing and supervision of the manuscript. All authors have read and approved the final manuscript.
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