2. Chemical methodologies of 2D c-MOFs
2765-2767Classifies monomers, linkages and notation systems for benzene, triphenylene and larger 2D c-MOF families.
Relevance: Core · p. 2766 · 2. Chemical methodologies of 2D c-MOFs · Fig. 2
Mingchao Wang, Renhao Dong and Xinliang Feng · Chem. Soc. Rev. · 2021
Review the chemistry, synthetic methodologies, structure-electronic property relationships, charge transport properties, device integration and MOFtronics functions of two-dimensional conjugated MOFs.
The review’s argument is preserved as a navigable set of section summaries.
Classifies monomers, linkages and notation systems for benzene, triphenylene and larger 2D c-MOF families.
Relevance: Core · p. 2766 · 2. Chemical methodologies of 2D c-MOFs · Fig. 2
Discusses bulk pellets, single-crystal devices, top-down exfoliation and bottom-up nanosheet synthesis for device integration.
Relevance: Core · p. 2779 · 5. Device integration based on multi-dispersed 2D c-MOFs · Figs. 17-18
Reviews electronic, optoelectronic, spintronic, thermoelectric and electrochemical energy-storage functions enabled by conductive 2D c-MOFs.
Relevance: Supporting · p. 2779 · 6. Functions for MOFtronics
Frames conductive MOFs and defines 2D c-MOFs as layer-stacked frameworks with in-plane extended conjugation and MOFtronics relevance.
Relevance: Core · p. 2765 · 1. Introduction · Fig. 1
Summarises performance advances while stressing limits in comparison metrics, layer-number control, crystallinity, device fabrication and controlled synthesis.
Relevance: Core · p. 2787 · 7. Conclusions and outlook
Synthesises how ligand type, geometry, metal identity, redox state, stacking and crystallinity influence carrier generation, band structure and measured transport.
Relevance: Core · p. 2767 · 3. Chemical structure and electronic property relationship in 2D c-MOFs · Table 1
Compares bulk hydro-/solvothermal methods, wet interfacial film growth, Langmuir-Blodgett routes and on-surface synthesis.
Relevance: Core · p. 2774 · 4. Synthetic methodologies of 2D c-MOFs · Fig. 9
Classification systems are attributed to this review and are not treated as a global material registry.
The review distinguishes intrinsic in-plane and interlayer pathways from extrinsic hopping through boundaries and defects.
Categories: through-bond · extended conjugation · through-space · hopping
p. 2767 · 3. Chemical structure and electronic property relationship in 2D c-MOFs
Ligand symmetry maps onto lattice geometry, which the review links to band-structure features such as Dirac points, flat bands and possible topological states.
Categories: hexagonal lattice · square lattice · honeycomb lattice · kagome metal-atom sublattice
p. 2769 · 3.2 Effect of ligand geometry · Figs. 4-5
The review uses linkage chemistry to organise 2D c-MOF families and to interpret differences in pi-d hybridisation and transport.
Categories: metal-bis(dioxolene) MO4 · metal-bis(diimine) MN4 · metal-bis(dithiolene) MS4 · metal-diimine-dithiolene MN2S2 · metal-bis(diselenolene) MSe4
p. 2766 · 2. Chemical methodologies of 2D c-MOFs · Fig. 2
Applications are grouped around electronic transport, sensing, magnetic/spintronic phenomena and electrochemical energy storage.
Categories: field-effect transistors · superconductors · chemiresistors · photodetectors · spintronics · thermoelectrics · metal-ion batteries · supercapacitors
p. 2779 · 6. Functions for MOFtronics
The review organises synthesis by whether it yields bulk particles/crystals, large-area films or processible nanosheets.
Categories: bulk hydro-/solvothermal powders and crystals · gas-liquid interfacial films · liquid-liquid interfacial films · liquid-solid interfacial films · Langmuir-Blodgett monolayers · top-down exfoliated nanosheets · bottom-up surfactant-assisted nanosheets
pp. 2774-2779 · 4-5 · Figs. 9, 11, 17
Review-defined families retain their representative materials and conduction descriptions.
2D c-MOFs incorporating mixed ligands or mixed metals within one framework to tune porosity, active sites and electronic structure.
Conduction: Mixed-metal HITP frameworks are used to demonstrate continuous conductivity changes with metal composition and interlayer displacement.
Representative materials: Cu3(HHTP)(HHB) · MnM'3-n(HITP)2
Nodes / linkers: Cu · Co · Ni · HHTP/HHB · HITP
p. 2771 · 3.3 Effect of metals · Fig. 6
2D c-MOFs using metal-bis(diimine) or metal-bis(iminobenzosemiquinoid) coordination, commonly from hexaaminobenzene or hexaaminotriphenylene linkers.
Conduction: MN4 systems are highlighted for improved charge transport relative to MO4 analogues and for processible FET and energy-storage devices.
Representative materials: Ni3(HITP)2 · Cu3(HITP)2 · Co3(HITP)2 · M3(HIB)2 · Ni2[CuPc(NH)8]
Nodes / linkers: Ni · Cu · Co · HAB/HIB · HATP/HITP · amino-phthalocyanine
p. 2767 · 3.1 Effect of ligand type · Table 1
2D c-MOFs based on metal-bis(dioxolene) linkages, typically from hydroxy-substituted benzene, triphenylene, phthalocyanine or related ligands.
Conduction: The review portrays MO4-linked systems as broadly conductive but generally inferior in charge transport to analogous MN4 and MS4 systems.
Representative materials: Cu3(HHTP)2 · Ni9(HHTP)4 · Cu3(HHB)2 · M2[M'PcO8]
Nodes / linkers: Cu · Ni · Co · Fe · Zn · HHB · HHTP · phthalocyanine · naphthalocyanine · DBC
pp. 2767-2768 · 3.1 Effect of ligand type · Table 1
2D c-MOFs based on metal-bis(dithiolene) linkages from thiol-substituted benzene, triphenylene or coronene ligands.
Conduction: MS4 linkages are described as having the highest pi-d hybridisation and some of the strongest reported conductivities and mobilities.
Representative materials: Cu3(HTB) · Ni3(HTB)2 · Fe3(HTTP)2 · Fe3(PTC)
Nodes / linkers: Cu · Ni · Fe · Co · Pt · BHT/HTB · THT/HTTP · PTC
p. 2767 · 3.1 Effect of ligand type · Table 1
Emerging selenium-analogue 2D c-MOFs with metal-bis(diselenolene) linkages.
Conduction: The review notes lower conductivity for reported MSe4-linked bulk examples than for MS4-linked bulk systems.
Representative materials: Cu3(HSeB) · Co3(HSeTP)2
Nodes / linkers: Cu · Co · HSeB · HSeTP
p. 2767 · 3.1 Effect of ligand type · Table 1
Few-layer nanosheets generated from bulk crystals or direct bottom-up nanosheet synthesis.
Conduction: Nanosheets are emphasised for solution processibility, accessible active sites and easier device integration rather than as intrinsic transport benchmarks.
Representative materials: Ni2[CuPc(NH)8] nanosheets · Cu3(HHB)2 nanosheets
Nodes / linkers: Ni · Cu · amino-phthalocyanine · HHB/THQ
p. 2779 · 5. Device integration based on multi-dispersed 2D c-MOFs · Fig. 18
Atomically thin 2D c-MOF layers pursued through Langmuir-Blodgett or on-surface methods.
Conduction: The review treats monolayers as central to intrinsic transport/topological questions, while noting that large single-crystalline monolayers are missing.
Representative materials: single-layer Ni3(HTTP)2 · monolayer Ni3(HITP)2 · monolayer Ni3(HTB)2
Nodes / linkers: Ni · Cu · HTTP · HITP · HTB
p. 2787 · 7. Conclusions and outlook
Review-level synthesis principles remain separate from primary-study recipes.
Surfactants restrict growth along the stacking direction and weaken interlayer interactions during direct nanosheet synthesis.
Claimed effects: Can produce single-crystalline, high-yield nanosheets with higher accessible surface area than bulk powders.
Controlling variables: surfactant identity · metal and ligand precursor concentrations · temperature · sonication · growth along c direction
Representative materials: Cu3(HHB)2 nanosheets
Caveat: Dispersion homogeneity, size/thickness/crystallinity control and restacking remain open process questions.
p. 2779 · 5. Device integration based on multi-dispersed 2D c-MOFs · Fig. 18
Solution heating of ligands and metal salts to form bulk powders, nanocrystals or moderate-sized single crystals.
Claimed effects: Scalable and high-yield family expansion, but commonly yields small polycrystalline particles that complicate processing and transport analysis.
Controlling variables: solvent · temperature · volume and pressure · base/deprotonation conditions · atmosphere and deoxygenation
Representative materials: Cu3(HHTP)2 · Ni3(HITP)2 · Fe2[FePcO8]
Caveat: Crystal growth is hard to monitor or control; small bulk polycrystals impede nanodevice integration and neat transport interpretation.
pp. 2774-2775 · 4.1 Bulk 2D c-MOFs through hydro-/solvothermal syntheses · Fig. 9
Ligands are compressed at the air/water interface and reacted with metal ions to form free-standing single-layer 2D c-MOF films.
Claimed effects: Targets large-area, free-standing single layers with high active-site exposure and processibility.
Controlling variables: surface pressure · ligand compression · metal-salt injection · transfer substrate · monolayer stability
Representative materials: single-layer Ni3(HTTP)2
Caveat: Successful examples remain limited and depend on soluble/selective building blocks and interfacial control.
p. 2777 · 4.2 2D c-MOF films through wet-interface-assisted synthesis · Fig. 14
Mechanical ball-milling or sonication delaminates bulk 2D c-MOF crystals into few-layer nanosheets.
Claimed effects: Improves solution processibility and active-site exposure while maintaining aspects of intrinsic porosity/conductivity.
Controlling variables: bulk crystal quality · milling energy · salt assistance · solvent dispersion · restacking during solidification
Representative materials: Ni2[CuPc(NH)8] nanosheets
Caveat: Limited control over morphology, layer number and lateral domain size.
p. 2779 · 5. Device integration based on multi-dispersed 2D c-MOFs · Fig. 17
Gas-liquid, liquid-liquid and liquid-solid interfacial routes that confine polymerisation and film formation at an interface.
Claimed effects: Can yield large-area thin films with better device integration and charge transport than dispersed bulk particles.
Controlling variables: interface type · ligand and metal salt concentration · reaction time · substrate · film thickness · orientation
Representative materials: Ni3(HTB)2 · Cu3(HTB) · Ni3(HITP)2 · Fe3(HTTP)2
Caveat: Universality, crystallinity, mechanical strength and thickness control remain unresolved.
p. 2776 · 4.2 2D c-MOF films through wet-interface-assisted synthesis · Fig. 11
These are the review authors’ synthesis, not newly measured results.
Crystallinity, grain boundaries, disorder and sample orientation strongly affect reported transport, so single-crystal or single-domain devices are needed for reliable intrinsic comparisons.
Evidence basis: multi_reference
Caveat: Review-table values span films, pellets, nanorods and nanosheets measured by different methods.
p. 2773 · 3.5 Effect of layer stacking and arrangement
2D c-MOFs are layer-stacked MOFs built from ortho-substituted conjugated building blocks and square-planar linkages, combining in-plane conjugation with weaker out-of-plane van der Waals interactions.
Evidence basis: review_reasoning
Caveat: The review notes that 3D MOFs can also be built from similar planar ligands, so layer-stacked structure is part of the definition.
p. 2765 · 1. Introduction
For batteries and supercapacitors, conductive 2D c-MOFs are promising but charge-storage mechanisms, ion/electron diffusion and binder/contact effects remain incompletely resolved.
Evidence basis: multi_reference
Caveat: Energy-storage performance examples should be treated as application context rather than direct evidence for intrinsic electronic conduction.
p. 2787 · 7. Conclusions and outlook
Hydro-/solvothermal methods are effective for expanding the material family but usually provide limited control over crystal growth and processability.
Evidence basis: review_reasoning
Caveat: The method can still produce important single-crystalline nanorods or nanoflakes in selected systems.
p. 2775 · 4.1 Bulk 2D c-MOFs through hydro-/solvothermal syntheses
Wet interfacial synthesis is presented as a route to large-area free-standing films that improve device integration and charge transport.
Evidence basis: multi_reference
Caveat: Applicable systems remain mainly benzene- or triphenylene-based, with unresolved film strength and thickness control.
p. 2788 · 7. Conclusions and outlook
Framework geometry is linked to electronic structure: honeycomb frameworks contain two distinct vertices and can host Dirac-point band features and kagome metal sublattices.
Evidence basis: multi_reference
Caveat: Several claims are theoretical or monolayer predictions rather than broad experimental demonstrations.
p. 2770 · 3.2 Effect of ligand geometry · Figs. 4-5
Layer stacking and interlayer interactions can change band structure and contribute substantially to cross-plane conductivity.
Evidence basis: multi_reference
Caveat: Stacking sequence must be resolved carefully; assumed AA/AB models can mislead band-structure interpretation.
p. 2772 · 3.5 Effect of layer stacking and arrangement · Fig. 8
Changing functional groups from O to NH to S generally strengthens metal-linker bonding and increases pi-d hybridisation, with MS4-linked systems showing especially strong conductivity/mobility examples.
Evidence basis: multi_reference
Caveat: The authors warn that the few examples, heterogeneous morphologies and possible doping make quantitative comparison difficult.
p. 2769 · 3.1 Effect of ligand type · Table 1
Metal substitution in M3(HITP)2 changes coordination geometry, layer spacing/displacement, bandgap and conductivity, enabling continuous tuning across mixed-metal networks.
Evidence basis: single_reference
Caveat: The review treats mixed-metal studies as promising but still limited in number.
p. 2771 · 3.3 Effect of metals · Fig. 6
Linkage redox state can inject or remove radical charge carriers, making redox activity a major design variable for conductivity.
Evidence basis: multi_reference
Caveat: Precise modulation and structural verification after redox reactions remain underdeveloped.
p. 2772 · 3.4 Effect of redox-activity in linkage · Fig. 7
The authors caution that 2D c-MOFs should not be judged by replacing silicon; comparisons must specify the property, device type and measurement technique.
Evidence basis: review_reasoning
Caveat: This is a review-level framing claim, not a primary benchmark.
p. 2786 · 7. Conclusions and outlook
Intrinsic conductivity is attributed mainly to in-plane through-bond/extended conjugation and out-of-plane through-space pi-pi/metal-metal interactions, whereas hopping is associated with grain boundaries and defects.
Evidence basis: multi_reference
Caveat: The review emphasises that real samples mix intrinsic and extrinsic contributions.
p. 2767 · 3. Chemical structure and electronic property relationship in 2D c-MOFs
Every row remains visibly secondary and links to a primary dossier only where the mapping is verified.
| Material | Property | Reported value | Context and quality | Primary evidence | Review source |
|---|---|---|---|---|---|
| SecondaryCu3(HHB)2 nanosheets | BET specific surface area | 385 m2 g-1 | Surfactant-assisted nanosheet synthesis with SDS; contrasted against powder sample. Text · Exact Reported | research_0043 | p. 2779 · 5. Device integration based on multi-dispersed 2D c-MOFs · Fig. 18 |
| SecondaryCu3(HTB) | field-effect mobility | 116 (e), 99 (h) cm2 V-1 s-1 | Film FET; electron and hole mobility reported in review Table 1. Table · Exact Reported | research_0006 | p. 2779 · 6.1.1 Field-effect transistors · Fig. 19 |
| SecondaryCu3(HTB) | electrical conductivity | 2500 S cm-1 | Film, 4-probe, room temperature; review Table 1. Table · Exact Reported | No verified corpus mapping | p. 2769 · 3.1 Effect of ligand type · Table 1 |
| SecondaryCu3(HTB) | superconducting transition temperature | 0.25 K | Electrical resistivity, AC magnetic susceptibility and specific heat measurements; transition disappears at 2500 Oe. Text · Exact Reported | No verified corpus mapping | p. 2780 · 6.1.2 Superconductors · Fig. 20 |
| SecondaryFe3(HTTP)2 | hole mobility | 229 (Hall, h) cm2 V-1 s-1 | Film, van der Pauw conductivity entry with Hall hole mobility in Table 1. Table · Exact Reported | research_0001 | p. 2769 · 3.1 Effect of ligand type · Table 1 |
| SecondaryFe3(HTTP)2 | TRTS mobility | 211 (TRTS) cm2 V-1 s-1 | Film, time-resolved terahertz spectroscopy mobility in review Table 1. Table · Exact Reported | research_0001 | p. 2769 · 3.1 Effect of ligand type · Table 1 |
| SecondaryFe3(PTC) | electrical conductivity | 10 S cm-1 | Pellet, van der Pauw, room temperature; review Table 1. Table · Exact Reported | research_0045 | p. 2769 · 3.1 Effect of ligand type · Table 1 |
| SecondaryMnM'3-n(HITP)2 mixed-metal series | composition-tuned conductivity | 0.024 to 55.4 S cm-1 | Co/Ni mixed-metal HITP system; increasing Ni content tunes layer distance/displacement and conductivity. Text · Range | research_0041 | p. 2771 · 3.3 Effect of metals · Fig. 6 |
| SecondaryNi2[CuPc(NH)8] nanosheets | nanosheet thickness | ~7 nm | NaCl-assisted low-energy ball milling; SEM/AFM/HR-TEM. Text · Approximate | No verified corpus mapping | p. 2779 · 5. Device integration based on multi-dispersed 2D c-MOFs · Fig. 18 |
| SecondaryNi3(HIB)2 | lithium-ion battery specific capacity | 155 mA h g-1 | Cathode material in 1 M LiPF6 electrolyte at 0.1 A g-1. Text · Exact Reported | No verified corpus mapping | p. 2783 · 6.5.1 Metal-ion batteries · Fig. 25 |
| SecondaryNi3(HITP)2 | EDL capacitor gravimetric capacitance | ~110 F g-1 | Pelletized Ni3(HITP)2, 1D channels, 0.05 A g-1 discharge rate. Text · Approximate | No verified corpus mapping | p. 2784 · 6.5.2 Supercapacitors · Fig. 26 |
| SecondaryNi3(HITP)2 | field-effect hole mobility | 48.6 cm2 V-1 s-1 | Film FET, p-type behaviour, as-synthesised sample. Text · Exact Reported | research_0015 | p. 2780 · 6.1.1 Field-effect transistors · Fig. 19 |
| SecondaryNi3(HITP)2 | electrical conductivity | up to ~60 S cm-1 | Polycrystalline 2D c-MOF, temperature-dependent semiconducting behaviour. Text · Approximate | No verified corpus mapping | p. 2773 · 3.5 Effect of layer stacking and arrangement |
| SecondaryNi3(HITP)2 | cross-plane electrical conductivity | up to 150 S cm-1 | Single-crystalline nanorod sample, cross-plane direction. Text · Approximate | research_0005 | p. 2773 · 3.5 Effect of layer stacking and arrangement |
| SecondaryNi9(HHTP)4 on laser-scribed graphene | micro-supercapacitor areal capacitance | 15.2 mF cm-2 | Hybrid interdigitated on 3D porous laser-scribed graphene. Text · Exact Reported | No verified corpus mapping | p. 2785 · 6.5.2 Supercapacitors · Fig. 27 |
Open questions are presented as review-author priorities, not conclusions from the primary database.
Compression and drop-casting of bulk materials limit reproducible, high-performance MOFtronic devices.
Proposed direction: Improve film quality, mechanical strength, smoothness, contacts and integration methods.
p. 2787 · 7. Conclusions and outlook
Boundaries, defects, edges and small domains obscure whether measured conductivity/mobility is intrinsic.
Proposed direction: Use reliable single-crystal or single-domain devices and control morphology/orientation before asserting structure-property relationships.
p. 2787 · 7. Conclusions and outlook
Hydro-/solvothermal synthesis barely controls crystal growth and often gives bulk samples that are hard to process.
Proposed direction: Design ligands/solvents and coordination reversibility to enlarge crystals, reduce defects and control morphology.
p. 2788 · 7. Conclusions and outlook
Interfacial synthetic methods are limited to a narrow set of systems and still face strength, orientation and size-control challenges.
Proposed direction: Broaden interfacial chemistry and tune thickness, lateral size, orientation and mechanical strength.
p. 2788 · 7. Conclusions and outlook
Current ligand design and linkage chemistry remain limited despite growth of the 2D c-MOF library.
Proposed direction: Expand rational ligand, linkage and multicomponent framework design while preserving conductivity and structural order.
p. 2787 · 7. Conclusions and outlook
Large single-crystalline monolayers needed for topological and heterostructure studies are still missing.
Proposed direction: Develop controlled chemical synthesis for large monolayers and van der Waals heterostructures.
p. 2787 · 7. Conclusions and outlook
Precise redox-state modulation and post-redox structural verification are underexplored, especially for negatively charged frameworks.
Proposed direction: Combine controlled redox chemistry with compositional and crystallographic checks to establish structure-conductivity relationships.
p. 2787 · 7. Conclusions and outlook
Functional studies remain concentrated on triphenylene-based systems, leaving other 2D c-MOF families underdeveloped.
Proposed direction: Extend MOFtronics testing across benzene, coronene, phthalocyanine and other linker families.
p. 2787 · 7. Conclusions and outlook
Mappings show which printed review references have a verified counterpart in the frozen primary corpus.
| Reference | Study | Role and context | Corpus mapping |
|---|---|---|---|
| Ref. 582020 | Title unavailable | mixed_metal · structure_property_relationship · conductivity_benchmarkCited for mixed-metal HITP frameworks, layer displacement and conductivity/bandgap tuning. | research_0041 |
| Ref. 1132015 | Title unavailable | band_structure · metal_substitution · stackingCited for DFT band-structure and stacking/metal-substitution interpretations of HITP frameworks. | Unmapped |
| Ref. 952019 | Title unavailable | single_crystal · conductivity_benchmark · stackingCited for single-crystalline nanorods/nanoflakes, stacking analysis and cross-plane transport discussion. | research_0005 |
| Ref. 452015 | Title unavailable | langmuir_blodgett · monolayer · electrocatalysis_contextCited for large-area free-standing single-layer 2D c-MOF synthesis and water-splitting context. | Unmapped |
| Ref. 322018 | Title unavailable | coronene_family · spintronics · conductivity_benchmarkCited for coronene-based MS4-linked Fe3(PTC), conductivity and ferromagnetic semiconductor discussion. | research_0045 |
| Ref. 782018 | Title unavailable | mobility_benchmark · photodetector · thin_film_synthesisCited for Fe3(HTTP)2 band-like transport, high mobility, interfacial film synthesis and photodetector application. | research_0001 |
| Ref. 402017 | Title unavailable | benzene_family · conductivity_benchmarkCited for MN4-linked M3(HIB)2 bulk samples and intrinsic metallicity in highly crystalline samples. | Unmapped |
| Ref. 2412020 | 10.1038/s41563-020-00847-710.1038/s41563-020-00847-7 | outlook · single_crystal_needCited in the outlook for the urgent need for single-crystals or single-domain monolayers. | Unmapped |
| Ref. 382018 | Title unavailable | pseudocapacitance · energy_storageCited for pseudocapacitor behaviour in MN4-linked benzene-based 2D c-MOFs. | Unmapped |
| Ref. 192012 | Title unavailable | first_2d_c_mof · synthesis_strategyCited as the first 2D c-MOF report and as the representative hydro-/solvothermal synthesis of TP-based MO4-linked materials. | Unmapped |
| Ref. 312015 | Title unavailable | fet_benchmark · wet_interface_synthesis · high_conductivityCited for Cu3(HTB) liquid-liquid interfacial film synthesis and ambipolar FET mobility. | research_0006 |
| Ref. 412018 | Title unavailable | ligand_family · dithioleneCited for benzenehexathiol/BHT ligand development and MS4-linked material family. | research_0735 |
| Ref. 682018 | Title unavailable | high_conductivity · superconductivityCited for very high Cu3(HTB) film conductivity and superconductivity measurements. | Unmapped |
| Ref. 742013 | Title unavailable | liquid_liquid_interface · film_synthesisCited as an early liquid-liquid interfacial 2D c-MOF film synthesis. | Unmapped |
| Ref. 752014 | Title unavailable | redox_activity · conductivity_benchmarkCited for redox modulation and conductivity changes in Ni3(HTB)2. | research_0361 |
| Ref. 392018 | Title unavailable | redox_activity · benzene_familyCited for negatively charged Cu3(HHB)2 and redox-state discussion. | research_0792 |
| Ref. 572014 | Title unavailable | ni_hitp_synthesis · conductivity_benchmarkCited for hydrothermal synthesis of Ni3(HITP)2 and polycrystalline conductivity behaviour. | Unmapped |
| Ref. 372017 | Title unavailable | supercapacitor_benchmark · energy_storageCited for EDL capacitor behaviour of pelletized Ni3(HITP)2. | Unmapped |
| Ref. 862020 | Title unavailable | topology · lattice_geometryCited for topology, lattice diagrams and geometry-band-structure discussion. | Unmapped |
| Ref. 362018 | Title unavailable | battery_benchmark · energy_storageCited for Ni3(HIB)2 as a Li-ion battery cathode and ligand-based redox interpretation. | Unmapped |
| Ref. 1122013 | Title unavailable | topological_state · theoryCited for predicted topological edge states in a Ni3(HTB)2 monolayer. | Unmapped |
| Ref. 552020 | Title unavailable | nanosheets · micro_supercapacitor · device_integrationCited for ball-milling exfoliation into nanosheets and flexible MSC device integration. | Unmapped |
| Ref. 882020 | Title unavailable | nanosheets · battery_benchmark · bottom_up_synthesisCited for surfactant-assisted single-crystalline Cu3(HHB)2 nanosheets and Li-ion battery performance. | research_0043 |
| Ref. 292017 | Title unavailable | fet_benchmark · thin_film_synthesisCited for Ni3(HITP)2 thin films and FET mobility/on-off performance. | research_0015 |
| Ref. 1002019 | Title unavailable | micro_supercapacitor · device_integrationCited for laser-scribed graphene-supported Ni9(HHTP)4 micro-supercapacitors. | Unmapped |
| Ref. 252020 | Title unavailable | transport_mechanism · review_contextCited for transport mechanisms and charge-transport characterisation context in conductive MOFs. | Unmapped |
| Ref. 332019 | Title unavailable | synthesis_strategy · phthalocyanine_family · magnetismCited for vacuum-promoted synthesis of oxygen-sensitive phthalocyanine 2D c-MOFs and ferromagnetic Fe2[FePcO8]. | research_0267 |
| Ref. 1262017 | Title unavailable | superconductivity_theoryCited for calculated superconducting transition temperatures for monolayer and bulk Cu3(HTB). | Unmapped |