2D Materials
22342-22343Surveys graphene, TMDs and MXenes to show that preparation, dimensionality and interlayer distance can change the sign, magnitude and mechanism of THz photoconductivity.
Relevance: Core · 22342 · 2D Materials
Jacob A. Spies, Jens Neu, Uriel T. Tayvah, Matt D. Capobianco, Brian Pattengale, Sarah Ostresh, and Charles A. Schmuttenmaer · The Journal of Physical Chemistry C · 2020
Explain how pump-probe terahertz spectroscopy and THz data analysis reveal photoconductivity, mobility limits, electron-phonon coupling, carrier confinement and resonant low-energy phenomena in emerging materials.
The review’s argument is preserved as a navigable set of section summaries.
Surveys graphene, TMDs and MXenes to show that preparation, dimensionality and interlayer distance can change the sign, magnitude and mechanism of THz photoconductivity.
Relevance: Core · 22342 · 2D Materials
Identifies future needs: broader multi-THz bandwidth, higher SNR/dynamic range, 2D TRTS feasibility, flexible sample preparation and closer collaboration with theory.
Relevance: Core · 22343 · Conclusions and Outlook
Compares thin-film approximation, transfer-function analysis, Drude, Drude-Smith and Lorentzian oscillator descriptions, including artefact and model-selection caveats.
Relevance: Core · 22338 · Introduction to THz Data Analysis
Frames THz spectroscopy as a contact-free alternative to electrode-based measurements for emerging materials whose size, morphology or instability make contacts difficult or intrusive.
Relevance: Core · 22335 · Introduction
Reviews THz evidence for small-polaron limits and carrier confinement in photoelectrode oxides such as BiVO4 and alpha-SnWO4, with bandwidth implications for higher-frequency phonons.
Relevance: Core · 22340 · Metal Oxide Photoelectrodes
Covers redox-doped and intrinsically conductive MOFs, comparing OPTP/TRTS to Hall/DC methods and identifying sensitivity and sample-form issues for porous crystalline materials.
Relevance: Core · 22340-22341 · Metal-Organic Frameworks
Uses lead-halide perovskites to show how THz separates free carriers, phonons, excitons and electron-phonon interactions that govern mobility.
Relevance: Core · 22339 · Perovskite Solar Absorbers
Explains why THz accesses both high-frequency free-carrier conductivity and low-energy bound-charge phenomena such as phonons, polarons and excitons.
Relevance: Core · 22337 · Physical Properties in the THz Regime
Introduces THz experiment anatomy, delay lines, TDS, OPTP and TRTS measurement types, and maps observable physical phenomena to generation/detection bandwidth.
Relevance: Core · 22335-22336 · A Practical Course in THz Spectroscopy · Figures 1-2
Classification systems are attributed to this review and are not treated as a global material registry.
Distinguishes extraction of optical constants from subsequent mechanism fitting, with Drude-Smith used for hindered long-range transport and Lorentzian terms for resonances.
Categories: thin-film approximation · transfer-function approach · Drude model · Drude-Smith model · Lorentzian oscillator model
22338 · Introduction to THz Data Analysis
Contrasts robust high-SNR solid-state methods with broader but more complex air-based or organic-crystal methods.
Categories: ZnTe/LiNbO3 · GaP · DAST/DSTMS · air plasma/ABCD · photoconductive antennae · spintronic emitters
22337-22338 · Physical Properties in the THz Regime · Figure 2
The review's materials section uses four families to demonstrate how THz interpretation changes with lattice softness, oxide polarons, porous crystals and van der Waals layered systems.
Categories: metal halide perovskites · metal oxide photoelectrodes · metal-organic frameworks · 2D materials
22335 · Abstract
Classifies THz measurements into steady-state time-domain reference spectra, peak-amplitude optical-pump traces for carrier kinetics, and full differential-waveform scans for complex photoconductivity spectra.
Categories: THz-TDS · OPTP · TRTS
22336-22337 · Anatomy of a THz Experiment · Figure 1
Uses perovskites and oxides to separate material-intrinsic scattering and electron-phonon effects from morphology- or processing-induced transport barriers.
Categories: particle-particle scattering · electron-phonon interactions · polaron formation · exciton formation · grain size and grain boundaries · particle confinement
22337 · Physical Properties in the THz Regime
The review organises THz transport interpretation around simultaneous access to free-carrier conductivity and low-energy polarization or resonant features.
Categories: free-carrier high-frequency conductivity · bound-charge dielectric response · phonons · polarons · excitons
22337 · Physical Properties in the THz Regime · Figure 2
Review-defined families retain their representative materials and conduction descriptions.
Atomically thin sheet materials stacked by van der Waals forces, with preparation-sensitive photoconductivity and broad electronic behaviour.
Conduction: Synthetic effects such as substrate doping can change the sign of THz transmission change, making fabrication history central to transport interpretation.
Representative materials: graphene · few-layer epitaxial graphene · 2D heterostructures
Nodes / linkers: Not specified · Not specified
22342 · 2D Materials
Semiconductor solar absorbers with strong absorption, long recombination lifetime and high nominal mobility, but with mobility often limited by electron-phonon, polaron and exciton effects.
Conduction: THz probes free-carrier photoconductivity, phonon modes, exciton dynamics and electron-phonon coupling that influence mobility.
Representative materials: CsPbBr3 · FA0.85Cs0.15Pb(I0.97Br0.03)3 · CH3NH3PbI3 · lead-halide perovskites
Nodes / linkers: Not specified · Not specified
22339 · Perovskite Solar Absorbers
Stable oxide photoanodes for oxidation reactions whose useful stability is offset by poor carrier mobility and small-polaron or confinement effects.
Conduction: Low mobility is discussed through small-polaron formation, lattice-vibration signatures, grain boundaries and suppressed low-frequency conductivity.
Representative materials: BiVO4 · alpha-SnWO4 · hematite · BiFeO3 · SnO2
Nodes / linkers: Not specified · Not specified
22340 · Metal Oxide Photoelectrodes
Highly ordered, porous materials made of organic linkers and inorganic metal nodes; usually insulating unless conductive channels or redox intercalation are introduced.
Conduction: THz can resolve subpicosecond photoconductivity, distinguish local optically excited transport from DC transport, and probe low-frequency framework motions.
Representative materials: HKUST-1 · Cu[Ni(pdt)2] · Fe3(THT)2(NH4)3 · Zn2TTFTB · ZIF-8
Nodes / linkers: Cu · Ni · Fe · Zn · benzenetricarboxylate · pyrazine-dithiolate · triphenylenehexathiol · tetrathiafulvalene tetrabenzoate · imidazolate
22340 · Metal-Organic Frameworks
2D layered metal carbides or nitrides formed by removing the A-site element from MAX phases and carrying surface terminations.
Conduction: THz distinguishes metallic from semiconductor-like response and can separate intra-nanosheet dark conductivity from inter-nanosheet photoconductivity.
Representative materials: Ti3C2Tz · Mo2Ti2C3Tz · Mo2TiC2Tz
Nodes / linkers: Ti · Mo · carbide · surface terminations
22342 · 2D Materials
Layered 2D semiconductors including MoS2 and WSe2, often relevant to batteries, photocatalysts and excitonic/trionic low-energy features.
Conduction: TRTS/OPTP can compare layer-dependent lifetimes and model photoconductivity with Drude plus Lorentzian exciton/trion terms.
Representative materials: 2H-MoS2 · monolayer MoS2 · trilayer MoS2 · WSe2
Nodes / linkers: Mo · W · sulfide · selenide
22342 · 2D Materials
Review-level synthesis principles remain separate from primary-study recipes.
Design conductive MOF structures rather than relying on insulating porous frameworks, using metal-node and linker choices to support charge transport.
Claimed effects: Enables band-like or high-mobility transport in selected semiconducting 2D MOFs and makes TRTS/Hall comparisons meaningful.
Controlling variables: metal node · organic linker · framework dimensionality · stacking order
Representative materials: Fe3(THT)2(NH4)3 · Zn2TTFTB
Caveat: Free-standing oriented films are difficult and limited to few MOFs; powder measurements may be more general but have signal challenges.
22340-22341 · Metal-Organic Frameworks
Use non-contact THz geometries with powders, thin films, pellets or nanoparticle suspensions when conventional contacts are difficult.
Claimed effects: Extends transport screening to emerging materials not readily compatible with electrodes while preserving native morphology better than contact fabrication.
Controlling variables: sample geometry · film thickness · pellet matrix · suspension medium · optical penetration depth
Representative materials: MOF powders · SnO2 thin films · nanoparticles in Nafion
Caveat: Data analysis must account for geometry and static optical parameters; signal may be weak in low-mobility materials.
22343 · Conclusions and Outlook
Use nanostructured morphologies so carriers are near the electrolyte interface, reducing the impact of intrinsically poor mobility.
Claimed effects: Can make limited mobility less consequential for holes at the interface but can introduce grain-boundary barriers for electrons reaching the back contact.
Controlling variables: particle size · grain-boundary density · electrode morphology · back-contact transport path
Representative materials: BiVO4 · alpha-SnWO4 · oxide nanoparticle photoanodes
Caveat: The cited Warren et al. nanostructure reference was not selected into key_cited_studies; the review uses the strategy as conceptual context rather than a benchmark.
22340 · Metal Oxide Photoelectrodes
Vacuum annealing removes solvent and cations, decreasing internanosheet distance and modifying photoconductivity dynamics.
Claimed effects: Annealed Mo2TiC2Tz shows increased long-time photoconductivity and a less negative Drude-Smith c-parameter, interpreted as higher internanosheet mobility.
Controlling variables: annealing temperature · annealing time · solvent content · inter-nanosheet distance · surface terminations
Representative materials: Mo2TiC2Tz · Mo2Ti2C3Tz
Caveat: The review interprets these as secondary evidence for structure-transport coupling rather than a universal MXene rule.
22342 · 2D Materials · Figure 5
Introduce redox-active species into otherwise insulating MOFs to create photoconductive behaviour measurable by OPTP.
Claimed effects: TCNQ- or iodine-intercalated MOFs become photoconductive and show ultrafast decay in OPTP.
Controlling variables: guest molecule · host framework · photoexcitation wavelength · pellet support
Representative materials: TCNQ@HKUST-1 · TCNQ@Cu[Ni(pdt)2] · I3@Cu[Ni(pdt)2]
Caveat: Conductivity is induced by guest species rather than necessarily intrinsic to the host framework.
22340 · Metal-Organic Frameworks
These are the review authors’ synthesis, not newly measured results.
For graphene and other 2D materials, preparation route and substrate effects can reverse the sign of photoinduced THz conductivity changes.
Evidence basis: multi_reference
Caveat: The review uses this as a warning against assuming transferable transport properties across nominally similar 2D samples.
22342 · 2D Materials
THz generation and detection involve a bandwidth-versus-SNR tradeoff: solid-state OR/EOS is robust and high field, while air-based and organic-crystal approaches provide broader bandwidth with practical complications.
Evidence basis: multi_reference
Caveat: Method choice depends on whether the target physics lies in low-frequency conductivity or higher-frequency resonances.
22337 · Physical Properties in the THz Regime
Mechanistic interpretation of THz transport in emerging materials increasingly requires collaboration between materials synthesis, spectroscopy and theory.
Evidence basis: single_reference
Caveat: This is an outlook claim rather than a quantitative evidence statement.
22343 · Conclusions and Outlook
Combining TRTS with femtosecond transient reflectance can separate two carrier mobilities in perovskites without contacts, but assignment to electrons versus holes requires outside knowledge.
Evidence basis: single_reference
Caveat: The two extracted mobilities are not species-labelled by the method alone.
22339 · Perovskite Solar Absorbers
THz spectroscopy is especially useful for emerging materials because it probes conductivity without contacts and can work across single crystals, polycrystalline flakes, amorphous materials and nanomaterials.
Evidence basis: multi_reference
Caveat: It probes local/high-frequency or photoexcited conductivity, not automatically the same quantity as long-distance DC transport.
22335 · Introduction
A negative Drude-Smith c-parameter is treated as evidence for hindered long-range transport, often associated with grain or particle boundaries.
Evidence basis: multi_reference
Caveat: The review notes the model is phenomenological, so c-parameter interpretation should be checked against morphology and complementary measurements.
22338 · Introduction to THz Data Analysis
The review identifies broader multi-THz bandwidth and ultrahigh-SNR dynamic-range spectrometers as necessary for next-generation material studies.
Evidence basis: multi_reference
Caveat: Broader bandwidth often competes with sensitivity, especially for low-mobility oxide and MOF samples.
22343 · Conclusions and Outlook
Suppressed low-frequency THz or microwave conductivity can indicate carrier confinement by particle or grain boundaries in nanostructured photoelectrodes.
Evidence basis: single_reference
Caveat: This interpretation must be separated from polaron formation and other low-mobility mechanisms.
22340 · Metal Oxide Photoelectrodes
For metal oxide photoelectrodes, small-polaron formation and low-frequency lattice modes are framed as key causes of poor photoconductivity and carrier mobility.
Evidence basis: multi_reference
Caveat: Other structural methods and computation are needed to assign the precise lattice vibration and guide compositional fixes.
22340 · Metal Oxide Photoelectrodes
The review claims THz methods are uniquely capable of measuring subpicosecond photoconductivity in MOFs, making them important for engineering photoconductive porous frameworks.
Evidence basis: multi_reference
Caveat: MOF signals can be weak and sample forms vary strongly between free-standing films and powders.
22340 · Metal-Organic Frameworks
In MXenes, combining THz-TDS and TRTS can separate intrinsic intrananosheet conductivity from photoinduced internanosheet transport affected by annealing and spacing.
Evidence basis: single_reference
Caveat: Evidence is from selected Mo-based MXenes and should not be generalised to all MXene compositions.
22342 · 2D Materials
OPTP is primarily a full-bandwidth peak-amplitude kinetics measurement, whereas TRTS scans the differential waveform at selected pump delays to obtain frequency-dependent complex photoconductivity.
Evidence basis: review_reasoning
Caveat: The authors warn that OPTP/TRTS naming conventions are used ambiguously in the literature.
22337 · Anatomy of a THz Experiment
In metal halide perovskites, THz spectroscopy can distinguish intrinsic electron-phonon/polaron/exciton effects from extrinsic grain-boundary limitations on mobility.
Evidence basis: multi_reference
Caveat: THz mobility often gives the electron-plus-hole sum unless combined with other measurements.
22339 · Perovskite Solar Absorbers
Unlike intensity-only spectroscopies, THz-TDS retrieves phase as well as magnitude, enabling complex optical parameters and conductivity to be extracted.
Evidence basis: single_reference
Caveat: Accurate extraction still requires appropriate geometry and reference measurements.
22336 · A Practical Course in THz Spectroscopy
The thin-film approximation is convenient but can fail when the photoexcited region is not sufficiently thin or when resonant features introduce artefacts.
Evidence basis: multi_reference
Caveat: Transfer-function analysis is more computational but described as practical on ordinary desktops.
22338 · Introduction to THz Data Analysis
TRTS-derived MOF photoconductivity and Hall/DC transport can differ because THz measurements include optical excitation, time resolution and local sampling.
Evidence basis: single_reference
Caveat: Comparison is informative but the two measurements are not interchangeable.
22341 · Metal-Organic Frameworks
The THz window is useful because it covers both femtosecond-picosecond carrier scattering and bound-charge phenomena such as phonons, polarons and excitons.
Evidence basis: multi_reference
Caveat: Not every material has resonant features within the accessible THz band of a given spectrometer.
22337 · Physical Properties in the THz Regime
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 |
|---|---|---|---|---|---|
| SecondaryAir plasma generation / ABCD detection | usable THz bandwidth | 0.3-30+ THz | Air-based multi-THz spectroscopy; ABCD requires high voltages. Text · Range | No verified corpus mapping | 22338 · Physical Properties in the THz Regime |
| SecondaryBiFeO3 | phonon mode frequency | ~3 THz | Review example of a metal-oxide phonon mode within broader THz reach. Text · Approximate | No verified corpus mapping | 22340 · Metal Oxide Photoelectrodes |
| SecondaryBiVO4 | carrier mobility example | ~0.4 cm2 V-1 s-1 | Review example of low carrier mobility in promising metal oxide photoelectrodes. Text · Approximate | No verified corpus mapping | 22340 · Metal Oxide Photoelectrodes |
| SecondaryBiVO4 | phonon bleach frequency | ~2 THz | TRTS studies of BiVO4 assigning phonon bleach to lattice distortion associated with polaron formation. Text · Approximate | No verified corpus mapping | 22340 · Metal Oxide Photoelectrodes |
| SecondaryDAST/DSTMS organic THz crystals | usable THz bandwidth | ~0.2-10+ THz | Organic OR/EOS crystals pumped often in near-infrared; review notes high fields and reliability concerns. Text · Range | No verified corpus mapping | 22337 · Physical Properties in the THz Regime |
| SecondaryFe3(THT)2(NH4)3 | THz conductivity versus DC conductivity | approximately an order of magnitude larger | TRTS Drude fits extrapolated to zero frequency compared with Hall-effect DC at room temperature. Text · Approximate | research_0001 | 22341 · Metal-Organic Frameworks |
| SecondaryGaP THz OR/EOS crystal | usable THz bandwidth | ~0.1-7 THz | Common solid-state generation/detection; broader than ZnTe due to higher-frequency phonon mode. Text · Range | No verified corpus mapping | 22337 · Physical Properties in the THz Regime |
| Secondaryhematite (alpha-Fe2O3) | phonons of interest frequency | as high as ~20 THz | Review example motivating larger bandwidth for metal oxide polaron studies. Text · Approximate | No verified corpus mapping | 22340 · Metal Oxide Photoelectrodes |
| SecondaryLiNbO3 THz source | usable THz bandwidth | ~0.1 to 2 THz | High-field THz generation via tilted-pulse-front pumping. Text · Range | No verified corpus mapping | 22337 · Physical Properties in the THz Regime |
| SecondaryCH3NH3PbI3 (MAPI) | multi-THz bandwidth used to observe exciton transitions | up to ~10 THz (~41 meV) | Air plasma generation and ABCD in ultrafast broadband multi-THz spectroscopy. Text · Approximate | No verified corpus mapping | 22339 · Perovskite Solar Absorbers |
| Secondary2H-MoS2 | trilayer versus monolayer ultrafast carrier lifetime | three times larger in the trilayer form | OPTP study of monolayer and trilayer 2H-MoS2 as summarised by the review. Text · Rounded Reported | No verified corpus mapping | 22342 · 2D Materials |
| Secondarymetal halide perovskites | exciton binding energy range | 3-41 meV (~0.7-10 THz) | Composition-dependent perovskite excitons as summarised by the review. Text · Range | No verified corpus mapping | 22339 · Perovskite Solar Absorbers |
| Secondarysolid-state biased coherent detection | broadband detection reach | out to ~10 THz | Commercially available broadband detection method discussed in outlook. Text · Approximate | No verified corpus mapping | 22343 · Conclusions and Outlook |
| SecondaryTCNQ@HKUST-1, TCNQ@Cu[Ni(pdt)2], I3@Cu[Ni(pdt)2] | ultrafast photoconductivity decay time | almost fully within 2 ps | OPTP with 400 nm photoexcitation on MOF samples pressed on polyethylene pellets. Text · Approximate | No verified corpus mapping | 22340 · Metal-Organic Frameworks |
| SecondaryZn2TTFTB | Drude-Smith c-parameter | -0.86 | TRTS Drude-Smith interpretation of conductive MOF powder photoconductivity. Text · Exact Reported | research_0030 | 22341 · Metal-Organic Frameworks |
| SecondaryZn2TTFTB | carrier scattering time from Drude-Smith fit | 17 fs | Frequency-dependent photoconductivity of as-prepared powder measured by TRTS according to the review paragraph. Text · Exact Reported | research_0030 | 22341 · Metal-Organic Frameworks |
| SecondaryZnTe THz OR/EOS crystal | usable THz bandwidth | ~0.1-3 THz | Common solid-state generation/detection with amplifier-based systems; review comparison against GaP. Text · Range | No verified corpus mapping | 22337 · Physical Properties in the THz Regime |
Open questions are presented as review-author priorities, not conclusions from the primary database.
The field needs systematic studies that separate interplane and intraplane conductivity in 2D materials and heterostructures.
Proposed direction: Use controlled pump/probe polarisation and ordered samples to probe specific 2D layer orientations and interlayer transport.
22343 · 2D Materials
Next-generation materials studies require larger bandwidth spectrometers to probe high-frequency resonant and dielectric phenomena that may limit charge transport.
Proposed direction: Develop and apply large-bandwidth multi-THz systems, including air-based and solid-state biased coherent detection approaches.
22343 · Conclusions and Outlook
TRTS carrier mobility measurements generally cannot separate electron and hole contributions on their own.
Proposed direction: Combine TRTS with transient reflectance, Hall measurements where feasible, calculations or prior literature to assign carrier species.
22339 · Perovskite Solar Absorbers
Mechanistic THz interpretation depends on collaboration between materials scientists, THz spectroscopists and theoreticians.
Proposed direction: Build collaborative workflows where state-of-the-art THz data are interpreted with material synthesis knowledge and theory.
22343 · Conclusions and Outlook
MOF THz studies need stronger photoconductivity or more sensitive instrumentation to extract carrier-density-dependent dynamics across pump fluence.
Proposed direction: Engineer more photoconductive MOFs and measure wide pump-fluence series with higher-sensitivity TRTS.
22341 · Metal-Organic Frameworks
Time-resolved photoinduced structural dynamics in crystalline MOFs are presented as a likely future application rather than an established area.
Proposed direction: Extend THz-TDS structural-mode studies to TRTS measurements of photoinduced framework dynamics.
22341 · Metal-Organic Frameworks
Low-mobility materials such as many metal oxides and MOFs produce weak TRTS signals, limiting practical mechanistic extraction.
Proposed direction: Improve ultrahigh-SNR, ultralow-noise and high-dynamic-range spectrometers and choose generation/detection methods carefully.
22340 · Metal Oxide Photoelectrodes
Thin-film approximations and resonant-feature artefacts can distort photoconductivity spectra.
Proposed direction: Use transfer-function analysis with accurate static parameters and known sample geometry when extracting complex refractive index changes.
22338 · Introduction to THz Data Analysis
Mappings show which printed review references have a verified counterpart in the frozen primary corpus.
| Reference | Study | Role and context | Corpus mapping |
|---|---|---|---|
| Ref. 22018 | Tutorial: An introduction to terahertz time domain spectroscopy (THz-TDS) | methods_background · data_analysisTutorial source used for THz-TDS definitions, transfer-function analysis and common bandwidth discussion. | Unmapped |
| Ref. 62020 | Suspensions of Semiconducting Nanoparticles in Nafion for Transient Spectroscopy and Terahertz Photoconductivity Measurements | sample_preparationCited as an example that THz-compatible sample preparation can extend to small-quantity nanoparticle suspensions. | Unmapped |
| Ref. 82018 | Applicability of the thin-film approximation in terahertz photoconductivity measurements | data_analysis · measurement_caveatUsed for the review's comparison of thin-film approximation and transfer-function analysis. | Unmapped |
| Ref. 92017 | Phonon features in terahertz photoconductivity spectra due to data analysis artifact: A case study on organometallic halide perovskites | data_analysis · artifact_caveatCited for the warning that resonant features can introduce artefacts in THz photoconductivity analysis. | Unmapped |
| Ref. 122019 | Coherent charge-phonon correlations and exciton dynamics in orthorhombic CH3NH3PbI3 measured by ultrafast multi-THz spectroscopy | perovskite · multi_thz · benchmarkUsed as the example of broadband multi-THz spectroscopy directly observing higher-energy exciton transitions in MAPI. | Unmapped |
| Ref. 132017 | Broadband terahertz pulse generation by optical rectification in GaP crystals | thz_generation · benchmarkSupports the review's comparison of GaP against ZnTe for broader THz bandwidth. | Unmapped |
| Ref. 142018 | The use of DSTMS crystal for broadband terahertz electro-optic sampling based on laser pulse amplitude changes | thz_detection · benchmarkSupports the review's statement that organic crystals such as DAST and DSTMS enable high-bandwidth THz measurements. | Unmapped |
| Ref. 152016 | A Broadband THz-TDS System Based on DSTMS Emitter and LTG InGaAs/InAlAs Photoconductive Antenna Detector | thz_generation · benchmarkAdditional cited support for DSTMS broadband THz-TDS instrumentation. | Unmapped |
| Ref. 162020 | Subcycle Nonlinear Response of Doped 4H Silicon Carbide Revealed by Two-Dimensional Terahertz Spectroscopy | outlook · advanced_thzUsed as an outlook example of state-of-the-art two-dimensional THz spectroscopy for emerging materials. | Unmapped |
| Ref. 172011 | Balanced terahertz wave air-biased-coherent-detection | thz_detection · benchmarkSource for the air-biased coherent detection bandwidth comparison and implementation caveat. | Unmapped |
| Ref. 212012 | A Review of the Terahertz Conductivity of Bulk and Nano-Materials | model_background · conductivity_reviewCited for physically motivated and phenomenological models of THz conductivity spectra. | Unmapped |
| Ref. 222001 | Classical generalization of the Drude formula for the optical conductivity | transport_model · drude_smithOriginal Drude-Smith model reference used to interpret confined or backscattered carrier transport. | Unmapped |
| Ref. 232017 | Microscopic origin of the Drude-Smith model | transport_model · grain_boundary_interpretationSupports the review's interpretation of Drude-Smith c-parameter as related to long-range transfer across grain or particle boundaries. | Unmapped |
| Ref. 242019 | Monitoring Electron-Phonon Interactions in Lead Halide Perovskites Using Time-Resolved THz Spectroscopy | perovskite · electron_phonon · benchmarkCentral perovskite example where TRTS separates carrier and phonon contributions and links deviations to exciton formation and breaking. | Unmapped |
| Ref. 252017 | Charge-Carrier Mobilities in Metal Halide Perovskites: Fundamental Mechanisms and Limits | perovskite · mobility_contextUsed by the review for the intrinsic/extrinsic mobility-limitation framing in perovskites. | Unmapped |
| Ref. 262020 | Polarons in Halide Perovskites: A Perspective | perovskite · polaron_context · benchmarkCited for perovskite polaron mechanisms and the range of exciton binding energies used in the review. | Unmapped |
| Ref. 272019 | Ultrafast THz Probe of Photoinduced Polarons in Lead-Halide Perovskites | perovskite · polaronUsed as the CsPbBr3 example where transient phonon-mode blue shifts are attributed to photoinduced polaron formation. | Unmapped |
| Ref. 302020 | Individual Electron and Hole Mobilities in Lead-Halide Perovskites Revealed by Noncontact Methods | perovskite · measurement_combinationCited for combining TRTS with fs-TR to extract two distinct mobilities without contacts. | Unmapped |
| Ref. 322016 | Ultrafast carrier dynamics in BiVO4 thin film photoanode material: interplay between free carriers, trapped carriers and low-frequency lattice vibrations | metal_oxide · polaron · benchmarkOne of the BiVO4 studies used to connect low-frequency lattice vibrations to poor carrier mobility. | Unmapped |
| Ref. 332016 | Direct Time-Resolved Observation of Carrier Trapping and Polaron Conductivity in BiVO4 | metal_oxide · polaron · benchmarkUsed for the review's BiVO4 mobility and polaron-conductivity discussion. | Unmapped |
| Ref. 372020 | Grain Boundaries Limit the Charge Carrier Transport in Pulsed Laser Deposited alpha-SnWO4 Thin Film Photoabsorbers | metal_oxide · grain_boundariesUsed as the metal-oxide example where THz and microwave comparison supports carrier confinement by grain boundaries. | Unmapped |
| Ref. 392020 | Effect of Doping and Excitation Wavelength on Charge Carrier Dynamics in Hematite by Time-Resolved Microwave and Terahertz Photoconductivity | metal_oxide · bandwidth_need · benchmarkCited for high-frequency hematite phonons that motivate multi-THz bandwidth for metal oxide polaron studies. | Unmapped |
| Ref. 402010 | Size-dependent infrared phonon modes and ferroelectric phase transition in BiFeO3 nanoparticles | metal_oxide · phonon_benchmarkCited for a BiFeO3 phonon mode frequency relevant to bandwidth choice. | Unmapped |
| Ref. 412020 | Electrically Conductive Metal-Organic Frameworks | mof · conductive_mof_contextCited for the broader statement that conductive channels can be engineered into MOF structures. | Unmapped |
| Ref. 422015 | Time-resolved terahertz spectroscopy of electrically conductive metal-organic frameworks doped with redox active species | mof · redox_intercalation · benchmarkFirst-generation OPTP example for redox-intercalated MOFs becoming photoconductive. | Unmapped |
| Ref. 432018 | High-mobility band-like charge transport in a semiconducting two-dimensional metal-organic framework | mof · transport_benchmarkCentral MOF example comparing TRTS-derived photoconductivity with Hall-effect transport. | research_0001 |
| Ref. 442012 | High charge mobility in a tetrathiafulvalene-based microporous metal-organic framework | mof · ttf_mofCited in the Zn2TTFTB paragraph; the review uses it around the powder-TRTS and time-resolved microwave comparison context. | research_0030 |
| Ref. 492009 | Broadband electromagnetic response and ultrafast dynamics of few-layer epitaxial graphene | 2d_materials · grapheneOne cited graphene study supporting the review's warning that preparation history alters THz response. | Unmapped |
| Ref. 502018 | Strong negative terahertz photoconductivity in photoexcited graphene | 2d_materials · grapheneContrasting graphene example where photoexcitation leads to negative THz photoconductivity. | Unmapped |
| Ref. 512014 | Ultrafast Transient Terahertz Conductivity of Monolayer MoS2 and WSe2 Grown by Chemical Vapor Deposition | 2d_materials · tmd · benchmarkUsed for TMD OPTP/TRTS examples including a longer ultrafast lifetime in trilayer MoS2 and trion modelling in WSe2. | Unmapped |
| Ref. 522014 | Trion-induced negative photoconductivity in monolayer MoS2 | 2d_materials · tmd · preparation_caveatContrasting MoS2 result showing decreased conductivity after photoexcitation under certain preparation procedures. | Unmapped |
| Ref. 532020 | Two-Dimensional MXenes Mo2Ti2C3Tz and Mo2TiC2Tz: Microscopic Conductivity and Dynamics of Photoexcited Carriers | 2d_materials · mxene · processingMXene example where THz-TDS/TRTS distinguish metallic and semiconductor-like behaviour and show annealing effects. | Unmapped |
| Ref. 552018 | Recent advances in the preparation, characterization, and applications of two-dimensional heterostructures for energy storage and conversion | 2d_materials · heterostructure_outlookUsed in the outlook for interlayer charge-transport questions in 2D heterostructures. | Unmapped |
| Ref. 562020 | Influence of Dye Sensitizers on Charge Dynamics in SnO2 Nanoparticles Probed with THz Spectroscopy | sample_preparation · nanoparticlesCited as an example of thin-film sample preparation in the review's conclusion. | Unmapped |
| Ref. 572017 | Solid-state-biased coherent detection of ultra-broadband terahertz pulses | outlook · bandwidth_benchmarkUsed as an outlook benchmark for commercially available broadband detection reaching about 10 THz. | Unmapped |
| Ref. 582019 | Collaboration between experiment and theory in solar fuels research | outlook · collaborationUsed to support the review's conclusion that material scientists, spectroscopists and theoreticians need to collaborate. | Unmapped |