Review · secondary evidenceReview

Conductive MOFs

Wen-Hua Li, Wei-Hua Deng, Guan-E Wang, Gang Xu · EnergyChem · 2020

This dossier represents secondary evidence: section summaries, claims and benchmarks are paraphrased for this database, not quoted. Check quantitative values against the linked primary study, and cite the review itself (10.1016/j.enchem.2020.100029) for its arguments.

11review sections
11material families
21review claims
22secondary benchmarks
40cited studies
10research gaps

Review scope

To summarise recent progress in electronically conductive and proton-conductive MOFs, emphasising material preparation, conductivity measurement, transport mechanisms, applications, and unresolved challenges.

Coverage
1979–2020
Category
Review Thermoelectric
Material scope
electronically conductive MOFs and PCPs · proton-conductive MOFs and PCPs · 2D pi-conjugated MOFs · doped and guest@MOF conductors · proton-conductive films and glass-state MOFs
Transport scope
through-space and through-bond electronic transport · hopping and band-like electronic transport · metallic and semiconducting states · Grotthuss and vehicular proton transport · humidity-mediated and anhydrous proton conduction
Application scope
chemiresistive sensing · supercapacitors and batteries · electrocatalysis · field-effect transistors and spintronic devices · thermoelectrics · fuel-cell electrolyte context
Explicit exclusions
ion-conductive MOFs other than proton conductors · proton-conducting MOF composites reviewed elsewhere · full experimental recipes and exhaustive bibliography
Source
p. 1 · Abstract
Evidence role
Context, taxonomy and secondary benchmarking

Section map

The review’s argument is preserved as a navigable set of section summaries.

2.5. Application

25-40

Surveys conductive MOFs in sensing, energy storage, energy conversion, electronics, spin valves, topological-insulator candidates and thermoelectrics.

Relevance: Core · p. 25 · 2.5. Application

2.2. Composition and crystal structures

8-20

Organises electronic MOFs by ligand and transport architecture, including planar multidentate ligands, pi-stacked pathways, redox/mixed-valence frameworks, metal-sulfur motifs, doped MOFs and guest@MOFs.

Relevance: Core · p. 8 · 2.2. Composition and crystal structures

2.4. Mechanism of the electronically conducting in MOFs

22-25

Distinguishes charge density and mobility, through-space/through-bond design, hopping/band models, and metallic-state examples.

Relevance: Core · p. 22 · 2.4. Mechanism

1. Introduction

1-2

Defines MOFs/PCPs, motivates conductivity as a limiting property, and frames electronic and proton conduction timelines.

Relevance: Core · pp. 1-2 · 1. Introduction · Schemes 1-2

2.3. Electrical transport measurements

20-22

Explains conductivity, thermal-variation and mobility measurements, including the importance of geometry, contacts, anisotropy and sample quality.

Relevance: Core · p. 20 · 2.3. Electrical transport measurements

4. Challenges and perspectives

54-55

Synthesises advantages, unresolved gaps and design principles for electronic and proton-conductive MOFs.

Relevance: Core · p. 54 · 4. Challenges and perspectives

3. Proton-conductive MOFs

40-41

Frames proton-conductive MOFs against PEMFC/Nafion requirements and the need for tunable crystalline platforms.

Relevance: Supporting · p. 40 · 3. Proton-conductive MOFs

3.2. Mechanism of proton conducting in MOFs

40-41

Defines Grotthuss and vehicular proton mechanisms and links activation energy to mechanistic assignment.

Relevance: Core · p. 40 · 3.2. Mechanism · Fig. 49

3.3. Proton sources in MOFs

41

Classifies proton sources as pore counterions, dangling acid groups, and protic guests/nonvolatile acids.

Relevance: Core · p. 41 · 3.3. Proton sources · Fig. 50

3.4. Types of proton-conductive MOFs

41-54

Organises proton-conductive MOFs by hydrous, anhydrous, dual-condition, film and glass-state systems.

Relevance: Supporting · p. 41 · 3.4. Types of proton-conductive MOFs

2.1. Synthesis methods

3-8

Compares hydro/solvothermal synthesis with interface-assisted methods for crystals, powders, thin films and single layers.

Relevance: Core · p. 3 · 2.1. Synthesis methods

Taxonomies

Classification systems are attributed to this review and are not treated as a global material registry.

Chemical And Physical Description Of Charge Transport

Electronic transport modes

The review explicitly presents a two-axis framework: chemical pathways through space/bond and physical mechanisms hopping/band-like.

Categories: through space · through bond · hopping · band theory

p. 22 · 2.4.1 · Fig. 24

Dominant Mobile CarrierAuthor-proposed

Conductive MOF scope

The review divides conductive MOFs into electronic charge conductors and proton conductors with separate mechanisms, measurements and applications.

Categories: electronically conductive MOFs · proton-conductive MOFs

p. 2 · 1. Introduction

Growth Interface And Device-Integration RouteAuthor-proposed

Interface-assisted synthesis routes

Figure 1 classifies interface-assisted routes used to form conductive MOF films from micron to centimetre scale and few-layer thickness.

Categories: gas-liquid interfacial synthesis · liquid-liquid interfacial synthesis · Langmuir-Blodgett method · solid-liquid interfacial synthesis · self-sacrificial templates · self-assembly on solid surfaces

p. 3 · 2.1.2 · Fig. 1

2D Network TopologyAuthor-proposed

Benzene-derived lattice motifs

For benzene-derived linker MOFs, the review distinguishes porous hexagonal networks from non-porous Kagome lattices.

Categories: hexagonal lattice with M-X4 planar metal sites · Kagome structure with continuous lateral connection

p. 11 · 2.2.1 · Fig. 11

Electrical Measurement Geometry And Sample Type

Conductivity measurement methods

The review connects choice of measurement to conductivity magnitude, contact resistance, thin-film geometry and sample anisotropy.

Categories: two-contact probe · four-contact probe · four-point method · van der Pauw method

p. 21 · 2.3.1 · Fig. 23

Organic Ligand Core And Terminal Donor GroupAuthor-proposed

Planar multidentate ligand subclasses

The composition section groups highly conductive pi-conjugated 2D MOFs by planar ligand families and metal nodes.

Categories: benzene-derived · triphenylene-derived · phthalocyanine-derived · fused-ring hydrocarbons

p. 9 · 2.2.1 · Figs. 9-18

Mode Of Proton Motion

Proton conduction mechanisms

The proton section distinguishes proton hopping through hydrogen-bond networks from diffusion of solvated proton carriers.

Categories: Grotthuss mechanism · vehicular mechanism

p. 40 · 3.2. Mechanism · Fig. 49

Humidity And Temperature RegimeAuthor-proposed

Proton-conductive MOF operating classes

The review organises proton conductors by water assistance, anhydrous operation, dual functionality, membrane processing and glass-state behaviour.

Categories: aqueous condition below 100 C · anhydrous condition · both anhydrous and humidified conditions · proton-conductive MOF films · glass-state MOFs

p. 2 · 1. Introduction · Scheme 2

Location And Chemical Nature Of Proton CarriersAuthor-proposed

Proton source types

The review classifies proton sources by whether they are intrinsic counterions/framework acid groups or guest species in pores.

Categories: Type I pore counterions · Type II dangling acid functional groups · Type III protic guest molecules or nonvolatile acids

p. 41 · 3.3. Proton sources · Fig. 50

Material families

Review-defined families retain their representative materials and conduction descriptions.

Benzene-derived conductive MOFs

2D Films, Pellets And Nanosheets

2D MOFs based on compact benzene-derived linkers bearing hydroxyl, imino, thiol, amino-thiol or selenolate groups.

Conduction: Short linkers promote strong orbital overlap; topology may be hexagonal porous or Kagome-like nonporous.

Representative materials: Ni-BHT · Cu-BHT · Cu3HIB2 · Cu3HSB

Nodes / linkers: Cu · Ni · Pd · Pt · Ag · HHB · HIB · HTB/BHT · TTB · HSB

p. 9 · 2.2.1 · Fig. 10 and Table 1

Carboxylate and phosphonate proton-conductive MOFs

2D Layers, 3D Channels And 1D Inorganic Chains

MOFs using carboxylate or phosphonate frameworks with acid groups, imidazole/imidazolium guests or ordered phosphate chains.

Conduction: Acidic groups, guest carriers and H-bond chains tune hydrous and anhydrous proton transport.

Representative materials: In-IA-2D-1 · Im@NENU-3 · BUT-8(Cr)A · PCMOF-5 · ZrP

Nodes / linkers: In · Zn · Cr · Zr · isophthalate · imidazolium carboxylate · sulfonated dicarboxylate · phosphonate

p. 45 · 3.4.1

Doped MOFs and guest@MOFs

3D Porous Host Frameworks And Thin Films

Conductive composites where redox-active dopants or donor-acceptor guests introduce carriers or charge-transfer pathways.

Conduction: Guest/dopant interactions can oxidise/reduce framework units or bridge host nodes to dramatically enhance conductivity.

Representative materials: I2@Cu[Ni(pdt)2] · KxFe2(BDP)3 · TCNQ@Cu3(BTC)2 · NiCB@NU-1000 · C60@NU-901

Nodes / linkers: Cu · Ni · Fe · Zr · pdt · BDP · BTC · pyrene linkers

p. 19 · 2.2.3 · Fig. 22

Glass-state CPs/MOFs for proton conductivity

Amorphous/Glassy Materials Derived From Crystalline CPs

Melt-quenched or mechanically amorphised coordination polymers/MOFs whose glass state enhances proton dynamics and processability.

Conduction: Glass formation can weaken proton-limiting interactions, enhance acidity and create flexible proton pathways.

Representative materials: CdTz · a-CdTz-40 · a-CdTz-240 · a-CdTz-500 · melted imidazole phosphates

Nodes / linkers: Cd · Zn · triazole · phosphate · imidazole

p. 53 · 3.4.5 · Fig. 68

Metal-sulfur chain and plane MOFs

1D Chains To 2D Planes

Conductive MOFs containing extended (-M-S-)n chains or planes with strong metal-chalcogen orbital overlap.

Conduction: Sulfur coordination lowers hopping barriers and, when expanded to planes, supports dense charge-transfer pathways.

Representative materials: Fe2(DSBDC) · Mn2(DSBDC) · [Cu2(6-Hmna)(6-mn).NH4]n

Nodes / linkers: Fe · Mn · Cu · DSBDC · Hmna/mn sulfur ligands

p. 18 · 2.2.2 · Fig. 21

Oxalate-based proton-conductive MOFs

1D Water Chains, 2D Layers And 3D Channel Networks

Hydrous proton-conducting MOFs whose oxalate frameworks host water, ammonium or hydrophilic channels.

Conduction: Hydrogen-bond networks and water/protonated counterions mediate Grotthuss-like transport.

Representative materials: Fe(ox).2H2O · (NH4)2(adp)[Zn2(ox)3].nH2O · (NH4)4[MnCr2(ox)6].4H2O · [Eu2(CO3)(ox)2(H2O)2].4H2O

Nodes / linkers: Fe · Zn · Mn/Cr · Eu · oxalate · adipate co-linker

p. 41 · 3.4.1

Phthalocyanine-derived conductive MOFs

2D Layered Molecular Meshes

2D conductive MOFs using phthalocyanine macrocycles with amino or hydroxyl groups and metal-centred square lattices.

Conduction: Macrocyclic pi systems and metal linkages offer tunable conductivity, sensing, electrocatalysis and magnetic ordering.

Representative materials: NiPc-M · NiNPc-M · K3Fe2[PcFe-O8] · PcCu-O8-Co

Nodes / linkers: Ni · Cu · Fe · Co · octaamino phthalocyanine · octahydroxy phthalocyanine · naphthalocyanine derivatives

p. 12 · 2.2.1 · Fig. 14

2D pi-conjugated planar multidentate MOFs

Primarily 2D Layered Frameworks

Layered MOFs assembled from planar multidentate ligands and planar metal-complex nodes with delocalised pi electrons.

Conduction: In-plane metal-ligand conjugation and interlayer interactions can support high electrical conductivity, sometimes metallic or band-like behaviour.

Representative materials: Ni3HITP2 · Cu3HHTP2 · Cu-BHT · PTC-Fe

Nodes / linkers: Cu · Ni · Co · Fe · HITP · HHTP · BHT/HTB · perthiolated coronene

p. 8 · 2.2.1

Pi-stacked 3D conductive MOFs

3D Porous Frameworks With 1D Stacks

Frameworks where non-covalent pi-pi stacks of electroactive ligands create charge-transport pathways.

Conduction: Short intermolecular contacts and stacked donor units enable through-space mobility and large conductivity enhancements.

Representative materials: Zn2(TTFTB) · M2(TTFTB) · ANMOF-74

Nodes / linkers: Zn · Mn · Co · Cd · Mg · Ni · tetrathiafulvalene tetrabenzoate · anthracene dicarboxylate

p. 17 · 2.2.2 · Fig. 19

Redox-active and mixed-valence MOFs

3D Porous Frameworks And 2D Magnets

MOFs whose conductivity is controlled by ligand redox manifolds, mixed-valence metal nodes or their combination.

Conduction: Redox manifolds and partially oxidised metal centres create charge carriers and hopping/delocalisation pathways.

Representative materials: (NBu4)2Fe2(dhbq)3 · Fe2(BDT)3 · Fe(tri)2(BF4)x

Nodes / linkers: Fe · V · benzoquinone-derived ligands · triazolate · BDT

p. 17 · 2.2.2 · Fig. 20

Triphenylene-derived MOFs

2D Layered Frameworks And Films

Conductive MOFs based on HHTP, HITP, HTTP or HSTP triphenylene linkers.

Conduction: Extended planar linkers support pi-d conjugation, stacking-dependent transport and possible metallic or thermoelectric behaviour.

Representative materials: Ni3HITP2 · Cu3HHTP2 · Co3HTTP2 · Fe3HTTP2

Nodes / linkers: Ni · Cu · Co · Fe · lanthanides · HHTP · HITP · HTTP · HSTP

p. 11 · 2.2.1 · Fig. 12

Synthesis strategies

Review-level synthesis principles remain separate from primary-study recipes.

Air-liquid interfacial HITP film formation

Hydrophilic-to-hydrophobic ligand transitions and water-surface nucleation yield free-standing Ni3HITP2 films.

Claimed effects: Produces smooth, large-area crack-free Ni3HITP2 films for porous FETs and Li-S separators.

Controlling variables: ligand wettability transition · nucleation at water surface · film thickness · transfer/stamping conditions

Representative materials: Ni3HITP2 film · Ni3HITP2/PP membrane

Caveat: Device performance still depends on interface quality and film crystallinity.

p. 5 · 2.1.2 · Fig. 5

Guest-mediated charge transfer

Electron-deficient or redox-active guest molecules are incorporated into porous hosts to create donor-acceptor pathways.

Claimed effects: Can transform insulating MOFs into conductive guest@MOFs without rebuilding the host framework.

Controlling variables: guest redox level · host donor/acceptor sites · pore connectivity · guest loading

Representative materials: TCNQ@Cu3(BTC)2 · NiCB@NU-1000 · C60@NU-901

Caveat: Mechanisms and stability depend strongly on host-guest interaction strength.

p. 20 · 2.2.3

Hydro-/solvothermal crystal growth

Autoclave synthesis in aqueous/non-aqueous solutions increases solubility/reactivity and supports crystal growth for 3D and some 2D conductive MOFs.

Claimed effects: Can give high-yield, low-cost conductive MOF crystals but is sensitive to conditions and hard to observe in real time.

Controlling variables: temperature · pressure · solvent · surfactant additives · precursor concentration

Representative materials: M-CAT · Ni3HITP2 · M2(TTFTB) · PTC-Fe

Caveat: Sealed autoclaves impede real-time observation; process is energy-consuming and parameter-sensitive.

p. 3 · 2.1.1

Liquid-liquid and gas-liquid interfacial growth

Interfaces between immiscible liquid phases or liquid/air are used to form conductive MOF films and nanosheets with controlled thickness.

Claimed effects: Enables high-quality thin films and nanosheets for device integration.

Controlling variables: interface type · solvent choice · air sensitivity · temperature · reactant concentration · container size

Representative materials: Ni-BHT · Cu-BHT · Ag-BHT · M-HIB films

Caveat: Film crystallinity and intrinsic transport can be damaged by poor crystallinity, grain boundaries or air sensitivity.

p. 4 · 2.1.2

Langmuir-Blodgett monolayer growth

Sub-monolayer organic linkers are compressed at the air-water interface before metal ions diffuse from the subphase to coordinate single layers.

Claimed effects: Allows molecular-level control of single-layer conductive MOF films and very thin device layers.

Controlling variables: surface pressure · monomer packing density · metal ion diffusion · water subphase composition

Representative materials: Ni3HTTP2 · Cu-CAT-1

Caveat: Single-layer formation is specialised and may not directly address large-scale device robustness.

p. 5 · 2.1.2 · Fig. 6

Liquid-solid interface integration

Template bottom-up assembly, layer-by-layer liquid-phase epitaxy and vapour-assisted conversion grow conductive MOFs directly on electrodes/substrates.

Claimed effects: Integrates conductive MOFs into sensors, photovoltaic/FET substrates and supercapacitor electrodes.

Controlling variables: substrate chemistry · growth cycle count · template composition · vapour conversion conditions · orientation

Representative materials: Cu3HHTP2 · Ni-CAT · M-CAT-1

Caveat: Each method trades off structural control, preparation time and substrate compatibility.

p. 6 · 2.1.2

On-surface self-assembly

Single-layer conductive MOFs are assembled directly on metal surfaces and characterised by STM/DFT.

Claimed effects: Reveals sub-molecular structures, band gaps and possible topological phases in single-layer MOFs.

Controlling variables: metal substrate · surface adsorption · single-layer registry · charge transfer to substrate

Representative materials: Cu3(C6O6) · Ni3HITP2 on Au(111)

Caveat: Surface-bound phases may differ from free-standing or bulk materials.

p. 7 · 2.1.2 · Fig. 8

Proton carrier and pathway design

Proton conductivity is increased by adding counterions, dangling acid groups, guest carriers or ordered hydrogen-bond pathways.

Claimed effects: Creates hydrous or anhydrous proton transport routes and can improve fuel-cell-relevant conductivity.

Controlling variables: carrier concentration · pKa matching · humidity · ordered protic-site alignment · activation energy

Representative materials: (NH4)2(adp)[Zn2(ox)3].3H2O · Im@NENU-3 · ZrP · Cu-TCPP nanofilm

Caveat: Processability, stability and high-temperature operation remain limiting for PEMFC use.

p. 55 · 4. Challenges and perspectives

Redox doping of conductive MOFs

Oxidation or reduction of redox-active ligands/metal nodes introduces carriers and changes conductivity.

Claimed effects: Can enhance conductivity by orders of magnitude and tune spin/photo/magnetic behaviour.

Controlling variables: oxidant/reductant identity · doping level · redox-active framework unit · structural robustness

Representative materials: I2@Cu[Ni(pdt)2] · KxFe2(BDP)3 · ZnNDI

Caveat: Precise dopant-level control and doped-system robustness remain challenging.

p. 20 · 2.2.3

Review claims

These are the review authors’ synthesis, not newly measured results.

Author InterpretationHigh supportCaveat

High-temperature anhydrous proton-conductive MOFs are still rare; most reported examples operate below 200 C and below 0.01 S cm-1.

Evidence basis: review_reasoning

Caveat: This is review status as of 2020 and should be updated for any later thesis claims.

p. 51 · 3.4.2

Author InterpretationMedium supportTransport Mechanism

Band-like transport is emerging in semiconducting MOFs but requires well-dispersed bands, low scattering and high-quality structural order.

Evidence basis: single_reference

Caveat: The review notes that defects, impurities and boundaries lower scattering time and mobility.

p. 23 · 2.4.1

Consensus SummaryHigh supportDefinition Scope

Most MOFs are electrical or protonic insulators, so conductive MOF design is framed as enabling electronic, electrochemical and fuel-cell technologies.

Evidence basis: review_reasoning

Caveat: This is a review-level generalisation rather than a measured value for a specific framework.

p. 54 · 4. Challenges and perspectives

Author InterpretationHigh supportCaveat

Redox doping and guest@MOF strategies can strongly enhance conductivity, but dopant-level precision and robustness remain major limitations.

Evidence basis: multi_reference

Caveat: The review distinguishes doped MOFs from host-guest charge-transfer systems.

p. 20 · 2.2.3

Author InterpretationMedium supportApplication Relevance

The review interprets conductive MOFs as promising electrodes, separators or hosts for supercapacitors and batteries because conductivity and porosity can coexist.

Evidence basis: multi_reference

Caveat: Low surface area, fragile films and device-scale processing limit current applications.

p. 33 · 2.5.2

Author InterpretationHigh supportConsensus

The field needs coordinated synthesis, precise measurement, theory and computation to establish structure-property relationships for conductive MOFs.

Evidence basis: review_reasoning

Caveat: Outlook statement from review authors.

p. 55 · 4. Challenges and perspectives

Author InterpretationMedium supportMaterial Comparison

Glass-state CPs/MOFs are presented as promising because they combine processability with altered proton dynamics compared with crystals.

Evidence basis: single_reference

Caveat: The review gives representative examples rather than a broad performance survey.

p. 53 · 3.4.5

Author InterpretationMedium supportStructure Property Link

Metal-sulfur chains and planes are highlighted as a route to stronger orbital overlap and lower hopping barriers than oxygen analogues.

Evidence basis: multi_reference

Caveat: Generality beyond cited M-S examples requires more primary evidence.

p. 18 · 2.2.2

Consensus SummaryHigh supportMeasurement Interpretation

Conductivity values in MOFs are method- and sample-dependent; contact resistance, geometry, homogeneity and anisotropy must be recorded.

Evidence basis: review_reasoning

Caveat: Review warns that pressed pellets and polycrystalline films often obscure intrinsic transport.

p. 21 · 2.3.1

Author InterpretationMedium supportMaterial Comparison

Conductive MOFs are usually semiconductors, but several BHT/HIB/HTTP examples exhibit metallic signatures or metallic-like transitions.

Evidence basis: multi_reference

Caveat: Experimental metallicity can be masked by grain boundaries and structural disorder.

p. 23 · 2.4.2

Consensus SummaryHigh supportTransport Mechanism

Electronic conductivity in MOFs requires both high charge density and high carrier mobility; metal nodes and organic linkers can both provide carriers.

Evidence basis: review_reasoning

Caveat: Specific mechanisms depend on framework composition and sample quality.

p. 22 · 2.4

Author InterpretationHigh supportMaterial Comparison

The review treats 2D pi-conjugated planar multidentate MOFs as the most conductive known MOF family.

Evidence basis: multi_reference

Caveat: No regular relation is yet observed between PAH extension and electrical transport.

p. 8 · 2.2.1

Author InterpretationHigh supportCaveat

Practical PEMFC use is limited by membrane/processability issues because most proton-conducting MOFs are pellets or single crystals.

Evidence basis: multi_reference

Caveat: The review cites early nanofilm work but does not claim broad device readiness.

p. 52 · 3.4.4

Consensus SummaryHigh supportTransport Mechanism

The review uses activation energy as a diagnostic: Grotthuss transport generally has lower Ea than vehicular transport.

Evidence basis: review_reasoning

Caveat: Activation-energy assignment is a heuristic and must be supported by structural evidence.

p. 41 · 3.2

Consensus SummaryHigh supportStructure Property Link

High proton conductivity in MOFs depends on carrier concentration, motion entropy, three-dimensional pathways and low activation energy.

Evidence basis: review_reasoning

Caveat: Humidity and guest volatility can dominate practical performance.

p. 41 · 3.2

Consensus SummaryHigh supportTransport Mechanism

Redox-active ligands and mixed-valence metal centres can increase carrier density and enable hopping/delocalised transport.

Evidence basis: multi_reference

Caveat: Mixed-valence states must be stabilised without degrading framework order.

p. 18 · 2.2.2

Consensus SummaryHigh supportApplication Relevance

Conductive 2D MOFs are attractive chemiresistive sensors because high conductivity, porosity and modular metal/linker chemistry can convert adsorption into electrical signals.

Evidence basis: multi_reference

Caveat: Mechanistic insight into host-guest interactions remains incomplete.

p. 28 · 2.5.1

Author InterpretationHigh supportMeasurement Interpretation

Single-domain films and single crystals are identified as the best forms for intrinsic anisotropic charge-transport studies.

Evidence basis: review_reasoning

Caveat: Such samples are difficult to synthesise, especially for 2D conductive MOFs.

p. 21 · 2.3.1

Consensus SummaryHigh supportStructure Property Link

Terminal groups, metal centres, stacking modes, crystal orientation, crystallinity, grain boundaries and defects can dramatically alter transport in conductive MOFs.

Evidence basis: review_reasoning

Caveat: The review emphasises that simple ligand-size trends are insufficient.

p. 9 · 2.2.1

Author InterpretationMedium supportApplication Relevance

Conductive MOFs are promising thermoelectrics because they can combine crystalline electronic transport with low thermal conductivity from porous/nanostructured frameworks.

Evidence basis: multi_reference

Caveat: Reported ZT values remain modest relative to practical thermoelectrics.

p. 39 · 2.5.4

Consensus SummaryHigh supportTransport Mechanism

Pi-pi stacking provides through-space transport when neighbouring ligands have short contacts and good orbital overlap.

Evidence basis: multi_reference

Caveat: Stacking geometry must be experimentally and computationally resolved.

p. 17 · 2.2.2

Secondary benchmarks

Every row remains visibly secondary and links to a primary dossier only where the mapping is verified.

MaterialPropertyReported valueContext and qualityPrimary evidenceReview source
Secondarya-CdTz-500proton conductivity1.0 x 10^-4 S cm-1below glass crystallisation temperature; glass-state CP
Text · Exact Reported
No verified corpus mappingp. 53 · 3.4.5
Secondary(NH4)2(adp)[Zn2(ox)3].3H2Oproton conductivity8 x 10^-3 S cm-1 at 25 C and 85% RH25 C, 85% RH
Text · Exact Reported
research_0220p. 41 · 3.4.1
SecondaryAg5HTB / Ag-BHTelectrical conductivity250 S cm-1film, 4-probe, room temperature; review Table 1
Table · Exact Reported
research_0735p. 10 · 2.2.1 · Table 1
SecondaryCu-BHTelectron mobility116 cm2 V-1 s-1film FET at 300 K
Text · Exact Reported
research_0006p. 22 · 2.3.3
SecondaryCu3HTB / Cu-BHTelectrical conductivity1580 S cm-1film, 4-probe, room temperature; review Table 1
Table · Exact Reported
research_0006p. 10 · 2.2.1 · Table 1
SecondaryCu3HSBelectrical conductivity110 S cm-1pellet, 4-probe, room temperature; review Table 1
Table · Exact Reported
No verified corpus mappingp. 10 · 2.2.1 · Table 1
Secondary[Cu2(6-Hmna)(6-mn).NH4]nelectrical conductivity10.96 S cm-1single crystal, 4-probe; review Table 2/text
Text · Exact Reported
research_0104p. 19 · 2.2.2 · Fig. 21
SecondaryCu-TCPP nanofilmproton conductivity3.9 x 10^-3 S cm-1 at 98% RH25 C/ambient text context, 98% RH
Text · Exact Reported
No verified corpus mappingp. 53 · 3.4.4
SecondaryFe(ox).2H2Oproton conductivity1.3 x 10^-3 S cm-1 at 25 C and 98% RH25 C, 98% RH
Text · Exact Reported
No verified corpus mappingp. 41 · 3.4.1
SecondaryFe3(THT)2(NH4)3charge mobility~220 cm2 V-1 s-1TRTS/Hall effect; semiconducting 2D MOF
Text · Approximate
research_0001p. 22 · 2.3.3
SecondaryNi3HITP2electrical conductivity150 S cm-1single crystal, 4-probe, room temperature; review Table 1
Table · Exact Reported
research_0005p. 10 · 2.2.1 · Table 1
SecondaryNi3HITP2electrical conductivity40 S cm-1film, van der Pauw, room temperature; review Table 1
Table · Exact Reported
No verified corpus mappingp. 10 · 2.2.1 · Table 1
SecondaryNi3HITP2thermal conductivity0.21 W m-1 K-1thermoelectric MOF; room-temperature context
Text · Exact Reported
research_0072p. 40 · 2.5.4
SecondaryNi3HITP2normalised capacitance~18 microF cm-2EDLC electrode, 10000 cycles with 90% retention
Text · Approximate
No verified corpus mappingp. 29 · 2.5.2
SecondaryNi3HITP2thermoelectric ZT1.19 x 10^-3 at room temperatureroom temperature
Text · Exact Reported
research_0072p. 40 · 2.5.4
Secondaryoxidized Ni-BHTelectrical conductivity1.6 x 10^2 S cm-1 at 300 Koxidized film/nanosheet, 300 K
Text · Exact Reported
research_0361p. 23 · 2.4.2
SecondaryTCNQ@Cu3(BTC)2electrical conductivity0.07 S cm-1film/device; guest@MOF
Text · Exact Reported
research_0088p. 20 · 2.2.3
SecondaryTCNQ@Cu3(BTC)2thermoelectric ZT7 x 10^-5 at 25 C25 C thin film
Text · Exact Reported
research_0450p. 39 · 2.5.4
SecondaryTCNQ@Cu3(BTC)2Seebeck coefficient375 microV K-1thin film thermoelectric measurement
Text · Exact Reported
research_0450p. 39 · 2.5.4
SecondaryZn2(TTFTB)intrinsic charge mobility0.2 cm2 V-1 s-1FP-TRMC; pi-stacked MOF
Text · Exact Reported
research_0030p. 17 · 2.2.2
SecondaryZrP, (NH4)3[Zr(H2/3PO4)3]anhydrous proton conductivity1.45 x 10^-3 S cm-1 at 180 C180 C, anhydrous
Text · Exact Reported
No verified corpus mappingp. 52 · 3.4.3
SecondaryZrP, (NH4)3[Zr(H2/3PO4)3]proton conductivity1.21 x 10^-2 S cm-1 at 90 C and 95% RH90 C, 95% RH
Text · Exact Reported
No verified corpus mappingp. 52 · 3.4.3

Research gaps

Open questions are presented as review-author priorities, not conclusions from the primary database.

Sample quality and defects

High

High-quality single crystals and single-domain films are scarce, especially for 2D conductive MOFs, limiting intrinsic transport measurements.

Proposed direction: Develop synthesis and characterisation routes for defect-controlled crystals/films.

p. 54 · 4. Challenges and perspectives

Controlled doping

Medium

Doped conductive MOFs need better control of dopant level and robustness.

Proposed direction: Develop moderate, reversible and structurally benign doping strategies.

p. 20 · 2.2.3

Intrinsic electronic transport mechanisms

High

Fundamental understanding of electron-lattice interactions and charge pathways in MOFs remains limited.

Proposed direction: Combine high-quality experiments with precise theoretical calculations to resolve mechanisms.

p. 2 · 1. Introduction

Measurement comparability

High

Conductivity values vary with measurement method, geometry, contact resistance and sample morphology.

Proposed direction: Report current/voltage windows, geometry, contact scheme, anisotropy and sample quality consistently.

p. 20 · 2.3

PEMFC deployment

High

MOF proton conductors still need simultaneous high conductivity, stability, mechanical strength and membrane processability.

Proposed direction: Evaluate repeated hydration/dehydration, high-temperature operation and mechanical durability.

p. 55 · 4. Challenges and perspectives

Anhydrous proton conduction

High

Few MOFs combine high-temperature tolerance above 200 C with proton conductivity above 0.01 S cm-1.

Proposed direction: Design nonvolatile carrier systems and thermally stable frameworks for Nafion alternatives.

p. 51 · 3.4.2

Proton-conductor processability

High

Most proton-conductive MOFs remain pellets or single crystals rather than practical membranes.

Proposed direction: Advance oriented films, membranes and mixed-matrix approaches while preserving conductivity.

p. 52 · 3.4.4

Stability of electronic MOFs

High

Conductive MOFs can lack robustness under heat, pressure and acid/base conditions.

Proposed direction: Prioritise robust frameworks and stability testing under device-relevant conditions.

p. 54 · 4. Challenges and perspectives

Host-guest sensing mechanisms

Medium

Conductive MOF chemiresistor mechanisms and host-guest interactions are not fully characterised.

Proposed direction: Use in situ spectroscopy, computation and systematic analyte studies to identify adsorption-to-transport links.

p. 28 · 2.5.1

Conductivity-porosity trade-off

Medium

Many highly conductive MOFs have surface areas below 1000 m2 g-1, challenging multifunctional porous conductors.

Proposed direction: Design frameworks balancing accessible surface area with high orbital overlap and carrier density.

p. 54 · 4. Challenges and perspectives

Cited-study map

Mappings show which printed review references have a verified counterpart in the frozen primary corpus.

Show 40 cited-study records
ReferenceStudyRole and contextCorpus mapping
Ref. 132009Electroconductive porous coordination polymer Cu[Cu(pdt)2] composed of donor and acceptor building unitshistorical_origin · through_bond_transportReview identifies this as one of the earliest electronically conductive MOF/PCP reports and a through-bond example.research_0201
Ref. 232009Rational designs for highly proton-conductive metal-organic frameworksproton_benchmark · rational_designUsed for rational incorporation of proton carriers and two-dimensional H-bond networks in oxalate MOFs.research_0220
Ref. 252009High proton conductivity of one-dimensional ferrous oxalate dihydrateproton_benchmarkUsed as a water-assisted oxalate proton conductor benchmark.Unmapped
Ref. 462012New porous crystals of extended metal-catecholatesmaterial_family · benchmarkReview uses this study for extended metal-catecholate/HHTP conductive MOFs.Unmapped
Ref. 472014High electrical conductivity in Ni3(2, 3, 6, 7, 10, 11-hexaiminotriphenylene)2, a semiconducting metal-organic graphene analoguematerial_family · benchmarkCited for HITP-based conductive MOFs and conductivity/BET values in Table 1.Unmapped
Ref. 492012High charge mobility in a tetrathiafulvalene-based microporous metal-organic frameworktransport_benchmark · pi_stackKey through-space/pi-stacked MOF mobility example.research_0030
Ref. 532019Integration of a (-Cu-S-)n plane in a metal-organic framework affords high electrical conductivitybenchmark · metal_sulfur_planeExample of 2D Cu-S plane enabling high single-crystal conductivity.research_0104
Ref. 572013pi-conjugated nickel bis(dithiolene) complex nanosheethistorical_development · material_familyReview presents Ni-BHT as an early pi-conjugated nickel bis(dithiolene) nanosheet and metallic-state platform.Unmapped
Ref. 612015A two-dimensional pi-d conjugated coordination polymer with extremely high electrical conductivity and ambipolar transport behaviourbenchmark · thin_film_deviceCentral high-conductivity Cu-BHT thin-film and FET mobility case.research_0006
Ref. 622018Highly conducting neutral coordination polymer with infinite two-dimensional silver-sulfur networksbenchmark · metallic_stateSilver-sulfur network with high conductivity and metallic features.research_0735
Ref. 642017Metallic conductivity in a two-dimensional cobalt dithiolene metal-organic frameworkmetallic_state · material_familyReview uses this for metallic conductivity in triphenylene dithiolene MOFs.Unmapped
Ref. 652019Room temperature metallic conductivity in a metal-organic framework induced by oxidationmetallic_state · material_familyReview uses this for Fe-HTTP metallic-like behaviour induced by oxidation.Unmapped
Ref. 662017Porous field-effect transistors based on a semiconductive metal-organic frameworkthin_film_device · benchmarkAir-liquid interfacial Ni3HITP2 film and porous FET benchmark.research_0015
Ref. 672018Large-Area preparation of crack-free crystalline microporous conductive membrane to upgrade high energy lithium-sulfur batteriesthin_film_device · battery_separatorLarge-area conductive MOF membrane separator for Li-S batteries.Unmapped
Ref. 752017Layer-by-layer assembled conductive metal-organic framework nanofilms for room-temperature chemiresistive sensingsynthesis_strategy · thin_film_deviceLayer-by-layer liquid-phase epitaxy for oriented conductive MOF films.research_0115
Ref. 762019Oriented thin films of electroactive triphenylene catecholate-based two-dimensional metal-organic frameworkssynthesis_strategy · thin_film_deviceVapour-assisted conversion strategy for oriented M-CAT films.Unmapped
Ref. 822017Signature of metallic behavior in the metal-organic frameworks M3(hexaiminobenzene)2 (M = Ni, Cu)benchmark · metallic_stateHIB benchmark for metallic behaviour in M3HIB2 frameworks.Unmapped
Ref. 862019[Cu3(C6Se6)]n: the first highly conductive 2D pi-d conjugated coordination polymer based on benzenehexaselenolatebenchmark · selenolate_linkerBenzenehexaselenolate 2D pi-d conductive polymer benchmark.Unmapped
Ref. 892019Single crystals of electrically conductive two-dimensional metal-organic frameworks: structural and electrical transport properties10.1021/acscentsci.9b01006benchmark · single_crystal_transportSingle-crystal 2D conductive MOF transport benchmark.research_0005
Ref. 992015Electronic conductivity, ferrimagnetic ordering, and reductive insertion mediated by organic mixed-valence in a ferric semiquinoid metal-organic frameworkmixed_valence · magnetic_semiconductorMixed-valence semiquinoid MOF with conductivity and magnetic ordering.research_0186
Ref. 1002018Tunable mixed-valence doping toward record electrical conductivity in a three-dimensional metal-organic frameworkmixed_valence · benchmarkReview uses this for Fe mixed-valence tuning and conductivity enhancement.Unmapped
Ref. 1012010Conductivity, doping, and redox chemistry of a microporous dithiolene-based metal-organic frameworkdoped_mof · through_bond_transportIodine oxidation/doping example in a microporous dithiolene MOF.research_0203
Ref. 1032019A highly crystalline anthracene-based MOF-74 series featuring electrical conductivity and luminescencepi_stack · material_familyAnthracene MOF-74 pi-stacking route to enhanced conductivity.research_0165
Ref. 1072018Electron delocalization and charge mobility as a function of reduction in a metal-organic frameworkdoped_mof · mobility_benchmarkPotassium-reduced Fe2(BDP)3 example with anisotropic conductivity and mobility increase.research_0029
Ref. 1092014Tunable electrical conductivity in metal-organic framework thin-film devicesguest_mof · thermoelectric_benchmarkGuest-induced conductivity and thermoelectric benchmark in HKUST-1.research_0088
Ref. 1142014Redox control and high conductivity of nickel bis(dithiolene) complex pi-nanosheet: a potential organic two-dimensional topological insulatorredox_control · topological_insulatorRedox-controlled Ni-BHT conductivity and potential topological-insulator context.research_0361
Ref. 1172018High-mobility band-like charge transport in a semiconducting two-dimensional metal-organic frameworkmobility_benchmark · band_transportRecord band-like mobility case from TRTS/Hall measurements.research_0001
Ref. 1432015Chemiresistive sensor arrays from conductive 2D metal-organic frameworksapplication_context · sensing2D conductive MOF chemiresistive sensor arrays.research_0145
Ref. 1572017Conductive MOF electrodes for stable supercapacitors with high areal capacitanceapplication_context · supercapacitorConductive MOF electrode with high areal capacitance in EDLCs.Unmapped
Ref. 1612018Multielectron-Transfer-based rechargeable energy storage of two-dimensional coordination frameworks with non-innocent ligandsapplication_context · batteryNon-innocent ligand 2D framework for Li-ion cathode.Unmapped
Ref. 1872016Electrochemical oxygen reduction catalysed by Ni3(hexaiminotriphenylene)2application_context · ORRNi3HITP2 ORR electrocatalysis benchmark/context.research_0003
Ref. 2192015Thin film thermoelectric metal-organic framework with high seebeck coefficient and low thermal conductivitythermoelectric_benchmarkThin-film thermoelectric MOF benchmark.research_0450
Ref. 2202017A microporous and naturally nanostructured thermoelectric metal-organic framework with ultralow thermal conductivitythermoelectric_benchmarkMicroporous Ni3HITP2 thermoelectric benchmark.research_0072
Ref. 2462014Control of crystalline proton-conducting pathways by water-induced transformations of hydrogen-bonding networks in a metal-organic frameworkproton_pathway · water_adsorptionWater-induced phase and H-bond pathway control in oxalate MOF.research_0324
Ref. 2522014High proton conduction at above 100 C mediated by hydrogen bonding in a lanthanide metal-organic frameworkproton_benchmark · high_temperatureHumidity-independent high-temperature lanthanide oxalate proton conductor.Unmapped
Ref. 2592017Straightforward loading of imidazole molecules into metal organic framework for high proton conductionproton_guestImidazole-loaded MOF with guest-assisted proton conduction.Unmapped
Ref. 2612017A flexible metal-organic framework with a high density of sulfonic acid sites for proton conductionproton_benchmark · sulfonic_acid_sitesFlexible sulfonic-acid-rich MOF proton conductor.Unmapped
Ref. 2842018Unique proton transportation pathway in a robust inorganic coordination polymer leading to intrinsically high and sustainable anhydrous proton conductivityproton_benchmark · fuel_cellRobust inorganic coordination polymer with humidified and anhydrous proton transport and fuel-cell test.Unmapped
Ref. 2902013Superprotonic conductivity in a highly oriented crystalline metal-organic framework nanofilmproton_film · benchmarkHighly oriented proton-conductive MOF nanofilm benchmark.Unmapped
Ref. 2992016Glass formation of a coordination polymer crystal for enhanced proton conductivity and material flexibilityglass_state · proton_benchmarkGlass-state coordination polymer proton-conductivity benchmark.Unmapped