THz time-domain and optical-pump terahertz-probe spectroscopy, including photoconductivity fits.
Every source method stays verbatim. Subtypes retain distinctions such as ATR versus transmission IR, powder versus single-crystal diffraction, and two- versus four-contact transport.
The same technique may serve transport, electrochemistry, sensing or another scientific purpose.
Filter source method wording, sample context and scientific purpose.
85 measurements
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Ca-HHTP film sample · Thin Film · Fourier-transformed Delta sigma(omega) from OPTP; Drude-Smith model fitted real and imaginary photoconductivity at 298 K.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Ca-HHTP film sample · Thin Film · 2 kHz, 100 fs, 800 nm Ti:sapphire source; 400 nm pump from BBO; THz pulses 0-3 THz; THz/probe and pump spots approx. 1.0/4.0 mm; mechanical chopper at 1 kHz.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Co-HHTP film sample · Thin Film · Fourier-transformed Delta sigma(omega) from OPTP; Drude-Smith model fitted real and imaginary photoconductivity at 298 K.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Co-HHTP film sample · Thin Film · 2 kHz, 100 fs, 800 nm Ti:sapphire source; 400 nm pump from BBO; THz pulses 0-3 THz; THz/probe and pump spots approx. 1.0/4.0 mm; mechanical chopper at 1 kHz.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Cu-HHTP film sample · Thin Film · Fourier-transformed Delta sigma(omega) from OPTP; Drude-Smith model fitted real and imaginary photoconductivity at 298 K.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Cu-HHTP film sample · Thin Film · 2 kHz, 100 fs, 800 nm Ti:sapphire source; 400 nm pump from BBO; THz pulses 0-3 THz; THz/probe and pump spots approx. 1.0/4.0 mm; mechanical chopper at 1 kHz.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Mg-HHTP film sample · Thin Film · Fourier-transformed Delta sigma(omega) from OPTP; Drude-Smith model fitted real and imaginary photoconductivity at 298 K.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Mg-HHTP film sample · Thin Film · 2 kHz, 100 fs, 800 nm Ti:sapphire source; 400 nm pump from BBO; THz pulses 0-3 THz; THz/probe and pump spots approx. 1.0/4.0 mm; mechanical chopper at 1 kHz.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Ni-HHTP film sample · Thin Film · Fourier-transformed Delta sigma(omega) from OPTP; Drude-Smith model fitted real and imaginary photoconductivity at 298 K.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Ni-HHTP film sample · Thin Film · 2 kHz, 100 fs, 800 nm Ti:sapphire source; 400 nm pump from BBO; THz pulses 0-3 THz; THz/probe and pump spots approx. 1.0/4.0 mm; mechanical chopper at 1 kHz.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Zn-HHTP film sample · Thin Film · Fourier-transformed Delta sigma(omega) from OPTP; Drude-Smith model fitted real and imaginary photoconductivity at 298 K.
2026 · Structure and Electrical Transport Properties of Metal Cate-Cholate Frameworks: The Metal Center Matters†
Zn-HHTP film sample · Thin Film · 2 kHz, 100 fs, 800 nm Ti:sapphire source; 400 nm pump from BBO; THz pulses 0-3 THz; THz/probe and pump spots approx. 1.0/4.0 mm; mechanical chopper at 1 kHz.
2025 · 2D Rhodium-Isocyanide Frameworks
as-prepared SJTU-201 powder · Powder · dry N2-purged environment at room temperature; 800 nm Ti:sapphire laser; frequency-resolved photoconductivity globally fitted
2025 · 2D Rhodium-Isocyanide Frameworks
as-prepared SJTU-202 powder · Powder · dry N2-purged environment at room temperature; 800 nm Ti:sapphire laser; frequency-resolved photoconductivity globally fitted
2025 · 2D Rhodium-Isocyanide Frameworks
as-prepared SJTU-203 powder · Powder · dry N2-purged environment at room temperature; 800 nm Ti:sapphire laser; frequency-resolved photoconductivity globally fitted
2025 · Ammonia-Assisted Chemical Vapor Deposition Growth of Two-Dimensional Conjugated Coordination Polymer Thin Films
Fe-HHB-o CVD thin film without NH3 · Thin Film · OPTP on about 101 nm Fe-HHB-o supported on fused silica; 800 nm pump, about 50 fs pulse, dry N2.
2025 · Ammonia-Assisted Chemical Vapor Deposition Growth of Two-Dimensional Conjugated Coordination Polymer Thin Films
Fe-HHB-w NH3-assisted CVD thin film · Thin Film · OPTP on about 99 nm Fe-HHB-w supported on fused silica; 800 nm pump, about 50 fs pulse, about 1.3 mJ/cm2 pump fluence, dry N2.
2025 · Enhanced Electrical Conductivity by the Heavy Chalcogen Effect in Metal-Organic Frameworks
Cu-S-HHS interfacial film · Thin Film · Film on quartz, 400 nm pump from BBO; pump fluence 600 uJ/cm2 for dynamics; 0-3 THz probe; frequency-resolved photoconductivity at 290 K.
2025 · Enhanced Electrical Conductivity by the Heavy Chalcogen Effect in Metal-Organic Frameworks
Cu-Se-HHS interfacial film · Thin Film · Film on quartz, 400 nm pump from BBO; pump fluence 600 uJ/cm2 for dynamics; 0-3 THz probe; frequency-resolved photoconductivity at 290 K.
2025 · Enhanced Electrical Conductivity by the Heavy Chalcogen Effect in Metal-Organic Frameworks
Cu-Te-HHS interfacial film · Thin Film · Film on quartz, 400 nm pump from BBO; pump fluence 600 uJ/cm2 for dynamics; 0-3 THz probe; frequency-resolved photoconductivity at 290 K.
2025 · Highly Porous, Electrically Conductive Two-Dimensional Nickel–Hexaaminodehydrobenzoannulene Frameworks
Ni3(HI12)2 film on fused silica · Thin Film · thin films on fused silica; 800 nm excitation; fluence 472 uJ cm-2; transient complex mobility spectra at 0.4 ps fitted with Drude-Smith model
2025 · Highly Porous, Electrically Conductive Two-Dimensional Nickel–Hexaaminodehydrobenzoannulene Frameworks
Ni3(HI18)2 film on fused silica · Thin Film · thin films on fused silica; 800 nm excitation; fluence 539 uJ cm-2; transient complex mobility spectra at 0.4 ps fitted with Drude-Smith model
2025 · Selenium-Substitution Strategy for Enhanced Mobility, Tunable Bandgap, and Improved Electrochemical Energy Storage in Semiconducting Conjugated Coordination Polymers
Ag4TSHQ drop-cast film · Thin Film · 3.1 eV optical excitation; frequency-resolved complex photoconductivity at ca. 1 ps after maximum photoconductivity.
2025 · Selenium-Substitution Strategy for Enhanced Mobility, Tunable Bandgap, and Improved Electrochemical Energy Storage in Semiconducting Conjugated Coordination Polymers
Ag4TTHQ drop-cast film · Thin Film · 3.1 eV optical excitation; frequency-resolved complex photoconductivity at ca. 1 ps after maximum photoconductivity.
2025 · Unveiling high-mobility hot carriers in a two-dimensional conjugated coordination polymer
large-area Cu3BHT film on fused silica · Thin Film · ~50 fs pump pulses; 1.55 eV excitation; Nabs 2.7-19.1 x 10^14 cm^-2; THz probe ~1 ps; dry N2-purged transmission mode at room temperature.
2025 · Unveiling high-mobility hot carriers in a two-dimensional conjugated coordination polymer
large-area Cu3BHT film on fused silica · Thin Film · Complex THz photoconductivity at 0.5 ps and 5 ps after Delta sigma peak under 1.55 eV photoexcitation, Nabs = 0.6 x 10^15 cm^-2.
2025 · Unveiling high-mobility hot carriers in a two-dimensional conjugated coordination polymer
large-area Cu3BHT film on fused silica · Thin Film · Cu3BHT film in cryostat under vacuum below 1 x 10^-4 mbar; 1.55 eV excitation at Nabs = 0.4 x 10^15 cm^-2; Drude fits of temperature-dependent Delta sigma(omega).
2024 · Control of the Hydroquinone/Benzoquinone Redox State in High-Mobility Semiconducting Conjugated Coordination Polymers
drop-cast Ag4TTBQ THz film · Thin Film · Optical-pump THz-probe; 800 nm laser pulses in SI, main text notes 1.55 eV pulsed laser; dry N2; pump fluences 30-522 uJ/cm2; frequency-resolved photoconductivity at 1 ps after maximum.
2024 · Control of the Hydroquinone/Benzoquinone Redox State in High-Mobility Semiconducting Conjugated Coordination Polymers
drop-cast Ag4TTHQ THz film · Thin Film · Optical-pump THz-probe; 800 nm laser pulses in SI, main text notes 1.55 eV pulsed laser; dry N2; pump fluences 30-522 uJ/cm2; frequency-resolved photoconductivity at 1 ps after maximum.
2024 · Manipulating Photoconduction in Cu-Pyrene 1-D Coordination Nanosheets by Modulating Interlayer π-π Stacking
Cu-PTT nanosheet powder · Nanosheet · Powder sample in 3 um mylar tape cell; 400 nm optical excitation with 150 uJ pulse followed by time-delayed THz pulse; peak THz transmission versus delay time measured.
2024 · Manipulating Photoconduction in Cu-Pyrene 1-D Coordination Nanosheets by Modulating Interlayer π-π Stacking
Cu-tBuPTT nanosheet powder · Nanosheet · Powder sample in 3 um mylar tape cell; 400 nm optical excitation with 150 uJ pulse followed by time-delayed THz pulse; peak THz transmission versus delay time measured.
2024 · Tunable Charge Transport and Spin Dynamics in Two-Dimensional Conjugated Metal-Organic Frameworks
Ni3(HATI_H)2 black powder · Powder · 400 nm photoexcitation, photon energy 3.1 eV, absorbed fluence 760 microJ cm-2; room-temperature N2 environment.
2024 · Tunable Charge Transport and Spin Dynamics in Two-Dimensional Conjugated Metal-Organic Frameworks
Ni3(HATI_iPr)2 black powder · Powder · 400 nm photoexcitation, photon energy 3.1 eV, absorbed fluence 760 microJ cm-2; room-temperature N2 environment.
2024 · Tunable Charge Transport and Spin Dynamics in Two-Dimensional Conjugated Metal-Organic Frameworks
Ni3(HATI_nPr)2 black powder · Powder · 400 nm photoexcitation, photon energy 3.1 eV, absorbed fluence 760 microJ cm-2; room-temperature N2 environment.
2024 · Tunable Charge Transport and Spin Dynamics in Two-Dimensional Conjugated Metal-Organic Frameworks
Ni3(HATI_vPr)2 black powder · Powder · 400 nm photoexcitation, photon energy 3.1 eV, absorbed fluence 760 microJ cm-2; room-temperature N2 environment.
2024 · Two-Dimensional Conjugated Metal–Organic Frameworks with a Ring-in-Ring Topology and High Electrical Conductance
Co-DHHBTN thin film on fused silica/quartz · Thin Film · 400 nm pump, 0.66 mJ cm-2, 2 kHz Ti:sapphire system, dry-air purge at 1.0% humidity; frequency-resolved complex THz photoconductivity.
2024 · Two-Dimensional Conjugated Metal–Organic Frameworks with a Ring-in-Ring Topology and High Electrical Conductance
Cu-DHHBTN thin film on fused silica/quartz · Thin Film · 400 nm pump, 0.66 mJ cm-2, 2 kHz Ti:sapphire system, dry-air purge at 1.0% humidity; frequency-resolved complex THz photoconductivity.
2024 · Two-Dimensional Conjugated Metal–Organic Frameworks with a Ring-in-Ring Topology and High Electrical Conductance
Ni-DHHBTN thin film on fused silica/quartz · Thin Film · 400 nm pump, 0.66 mJ cm-2, 2 kHz Ti:sapphire system, dry-air purge at 1.0% humidity; frequency-resolved complex THz photoconductivity.
2023 · Conjugated Nonplanar Copper-Catecholate Conductive Metal-Organic Frameworks via Contorted Hexabenzocoronene Ligands for Electrical Conduction
c-HBC-12O-Cu film for OPTP · Thin Film · 800 nm femtosecond laser pulses; pump fluence about 1.3 mJ cm-2; dry N2; frequency spectra recorded about 0.5 ps after maximum photoconductivity.
2023 · Conjugated Nonplanar Copper-Catecholate Conductive Metal-Organic Frameworks via Contorted Hexabenzocoronene Ligands for Electrical Conduction
c-HBC-6O-Cu film for OPTP · Thin Film · 800 nm femtosecond laser pulses; pump fluence about 1.3 mJ cm-2; dry N2; frequency spectra recorded about 0.5 ps after maximum photoconductivity.
2023 · Conjugated Nonplanar Copper-Catecholate Conductive Metal-Organic Frameworks via Contorted Hexabenzocoronene Ligands for Electrical Conduction
c-HBC-8O-Cu film for OPTP · Thin Film · 800 nm femtosecond laser pulses; pump fluence about 1.3 mJ cm-2; dry N2; frequency spectra recorded about 0.5 ps after maximum photoconductivity.
2023 · Dominant Role of Hole Transport Pathway in Achieving Record High Photoconductivity in Two-Dimensional Metal–Organic Frameworks
Cu-HHTP tape-cell sample · Unknown · 400 nm pump; pump power 90 mW; THz probe; tape-cell samples thick enough to absorb pump pulse; time delay spanning 125 ps.
2023 · Dominant Role of Hole Transport Pathway in Achieving Record High Photoconductivity in Two-Dimensional Metal–Organic Frameworks
Cu/Zn-HHTP tape-cell sample · Unknown · 400 nm pump; same OPTP comparison and Table S2 exponential fit.
2023 · Dominant Role of Hole Transport Pathway in Achieving Record High Photoconductivity in Two-Dimensional Metal–Organic Frameworks
Zn-HHTP tape-cell sample · Unknown · 400 nm pump; same OPTP comparison and Table S2 exponential fit.
2023 · Dominant Role of Hole Transport Pathway in Achieving Record High Photoconductivity in Two-Dimensional Metal–Organic Frameworks
Cu-HHTP tape-cell sample · Unknown · Ground-state THz-TDS at 300, 200 and 100 K measured absorption coefficient, refractive index and permittivity.
2023 · Engineering Band Gap and Photoconduction in Semiconducting Metal Organic Frameworks: Metal Node Effect
M-THQ mylar tape cell series · Powder · 400 nm optical pump at 1 kHz, 110 mW; powdered M-THQ in 3 um mylar tape cell; Gaussian-convoluted single-exponential fit with long-time offset.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-CuPc thin film on fused silica · Thin Film · 800 nm/1.55 eV optical excitation; dry N2 transmission geometry; room temperature.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-CuPc powder · Powder · Powder sandwiched between two fused silica substrates to form tens-of-micrometre films.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-NiPc thin film on fused silica · Thin Film · 800 nm/1.55 eV optical excitation; dry N2 transmission geometry; room temperature.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-NiPc powder · Powder · Powder sandwiched between two fused silica substrates to form tens-of-micrometre films.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-CuPc thin film on fused silica · Thin Film · Cryostat under vacuum; 298 K to 78 K.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-NiPc thin film on fused silica · Thin Film · Cryostat under vacuum; 298 K to 78 K.
2023 · Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers
2DCP-NiPc thin film on fused silica · Thin Film · 1.55 eV pump excitation; photoconductivity decay fitted with two exponential components.
2023 · Near IR Bandgap Semiconducting 2D Conjugated Metal-Organic Framework with Rhombic Lattice and High Mobility
Cu2(OHPTP) powder between fused-silica windows, 280 um · Powder · 280 um Cu2(OHPTP) powder between fused silica windows at 300 K; non-contact frequency-resolved complex conductivity; ambient/nitrogen-flushed conditions.
2023 · Near IR Bandgap Semiconducting 2D Conjugated Metal-Organic Framework with Rhombic Lattice and High Mobility
Cu2(OHPTP) powder between fused-silica windows, 150 um, vacuum · Powder · 150 um powder in fused-silica windows measured under vacuum at 100, 150, 200, and 250 K.
2023 · Semiconducting Conjugated Coordination Polymer with High Charge Mobility Enabled by “4 + 2” Phenyl Ligands
Cu3BHT thin film on fused silica/SiO2 substrate · Thin Film · Same THz/OPTP measurements as Cu4DHTTB film; used as metallic control.
2023 · Semiconducting Conjugated Coordination Polymer with High Charge Mobility Enabled by “4 + 2” Phenyl Ligands
Cu4DHTTB thin film on fused silica/SiO2 substrate · Thin Film · 800 nm, about 50 fs, 1 kHz laser pulses; dry N2; pump fluences 29-79 uJ/cm2 for dynamics and 318 uJ/cm2 for frequency-resolved Drude fits at 10, 100 and 1000 ps.
2023 · Semiconducting Conjugated Coordination Polymer with High Charge Mobility Enabled by “4 + 2” Phenyl Ligands
Cu4DHTTB thin film on fused silica/SiO2 substrate · Thin Film · Temperature-dependent THz photoconductivity under vacuum pressure < 2 x 10-4 mbar with a cryostat.
2023 · Semiconducting Conjugated Coordination Polymer with High Charge Mobility Enabled by “4 + 2” Phenyl Ligands
Cu4DHTTB thin film on fused silica/SiO2 substrate · Thin Film · THz waveforms through blank SiO2, Cu3BHT and Cu4DHTTB films recorded without photoexcitation; Fourier transformed to obtain sigma(omega).
2022 · Precise tuning of interlayer electronic coupling in layered conductive metal-organic frameworks
Ni3(HATI_C1)2 black powder · Powder · Room-temperature dark THz-TDS in N2-purged box; samples deposited on mask; Drude-Smith model fit.
2022 · Precise tuning of interlayer electronic coupling in layered conductive metal-organic frameworks
Ni3(HATI_C3)2 black powder · Powder · Room-temperature dark THz-TDS in N2-purged box; samples deposited on mask; Drude-Smith model fit.
2022 · Precise tuning of interlayer electronic coupling in layered conductive metal-organic frameworks
Ni3(HATI_C4)2 black powder · Powder · Room-temperature dark THz-TDS in N2-purged box; samples deposited on mask; Drude-Smith model fit.
2021 · Cation-exchanged conductive Mn2DSBDC metal–organic frameworks: Synthesis, structure, and THz conductivity
Co@Mn2DSBDC powder · Powder · 20-30 mg MOF mixed with about 1 g Teflon/PTFE and pressed at 11 kbar; air, bare PTFE and sample transmission collected at each temperature; effective medium theory used.
2021 · Cation-exchanged conductive Mn2DSBDC metal–organic frameworks: Synthesis, structure, and THz conductivity
Cu@Mn2DSBDC powder · Powder · 20-30 mg MOF mixed with about 1 g Teflon/PTFE and pressed at 11 kbar; air, bare PTFE and sample transmission collected at each temperature; effective medium theory used.
2021 · Cation-exchanged conductive Mn2DSBDC metal–organic frameworks: Synthesis, structure, and THz conductivity
as-prepared Mn2DSBDC powder · Powder · 20-30 mg MOF mixed with about 1 g Teflon/PTFE and pressed at 11 kbar; air, bare PTFE and sample transmission collected at each temperature; effective medium theory used.
2021 · Cation-exchanged conductive Mn2DSBDC metal–organic frameworks: Synthesis, structure, and THz conductivity
Ni@Mn2DSBDC powder · Powder · 20-30 mg MOF mixed with about 1 g Teflon/PTFE and pressed at 11 kbar; air, bare PTFE and sample transmission collected at each temperature; effective medium theory used.
2020 · A conductive metal-organic framework photoanode
Zn2TTFTB-TiO2 photoanode · Electrode · Samples on quartz excited from the front at 400 nm with pump fluences 0.26, 0.51, 0.89 and 1.27 mJ cm-2; THz attenuation measured at peak THz pulse.
2020 · A conductive metal-organic framework photoanode
TTFTB-sensitized TiO2 · Electrode · Ligand-sensitized TiO2 control on quartz, excited at 400 nm at same pump fluences as Zn2TTFTB-TiO2.
2020 · A conductive metal-organic framework photoanode
Zn2TTFTB-ZrO2 control film · Thin Film · Zn2TTFTB-ZrO2 non-injecting control measured at 400 nm; highest fluence 1.27 mJ cm-2 discussed.
2020 · Direct Evidence of Photoinduced Charge Transport Mechanism in 2D Conductive Metal Organic Frameworks
Cu-THQ tape-cell sample for OPTP and THz-TDS · Powder · 400 nm optical pump from frequency-doubled 800 nm; THz generation from plasma source; detection by free-space electro-optic sampling in ZnTe (110); pump-probe traces and frequency-dependent photoconductivity.
2020 · Direct Evidence of Photoinduced Charge Transport Mechanism in 2D Conductive Metal Organic Frameworks
Cu/Zn-THQ tape-cell sample for OPTP and THz-TDS · Powder · 400 nm optical pump; OPTP traces compared with Cu-THQ; frequency-dependent signal too small for direct measurement.
2020 · Direct Evidence of Photoinduced Charge Transport Mechanism in 2D Conductive Metal Organic Frameworks
Zn-THQ tape-cell sample for OPTP control · Powder · Normalized OPTP traces for Zn-THQ control; used to assess through-space contribution.
2020 · Direct Evidence of Photoinduced Charge Transport Mechanism in 2D Conductive Metal Organic Frameworks
Cu-THQ tape-cell sample for OPTP and THz-TDS · Powder · 800 nm oscillator and photoconductive antennas; tape cells with empty tape-cell reference; data at 300, 200 and 100 K averaged over three temperatures, two samples per material and three locations per sample.
2019 · A semiconducting layered metal-organic framework magnet
K3Fe2[PcFe-O8] optical pump-THz probe sample · Thin Film · Optical pump-THz probe; 800 nm excitation, 300 uJ cm-2 pump fluence, ~1 THz centre frequency/bandwidth probe; nitrogen environment.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
As-prepared Zn2TTFTB tape-cell sample · Powder · 400 nm pump pulses; representative trace and four independent samples globally fit with Gaussian-convoluted triexponential function; IRF FWHM set to 0.6 ps.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
As-prepared Zn2TTFTB tape-cell sample · Powder · Powder X-ray diffraction after TRTS beam exposure.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
As-prepared Zn2TTFTB tape-cell sample · Powder · 400 nm pump from frequency-doubled Ti:sapphire amplifier; THz generated in two-colour air plasma and detected by electro-optical sampling in ZnTe.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
Blank tape cell reference · Model · Blank tape cell measured without Zn2TTFTB sample.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
As-prepared Zn2TTFTB tape-cell sample · Powder · Tape reference and two sample locations scanned with micropositioning stage to check sample homogeneity and preparation reproducibility.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
Zn2TTFTB tape cell pressed at 11 kbar · Pellet · Tape cell measured after applying 11 kbar pressure.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
Zn2TTFTB pressed PTFE pellet · Pellet · Pressed Zn2TTFTB/PTFE pellet measured after 11 kbar pressure.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
As-prepared Zn2TTFTB tape-cell sample · Powder · Complex frequency-dependent refractive index determined from sample, air reference and tape reference measurements.
2019 · Metal-Organic Framework Photoconductivity via Time-Resolved Terahertz Spectroscopy
As-prepared Zn2TTFTB tape-cell sample · Powder · Spectrally resolved photoconductivity measured 500 fs after 400 nm photoexcitation; 0.25-0.75 THz and >2 THz resonance regions excluded from Drude-Smith fit.
2018 · High-mobility band-like charge transport in a semiconducting two-dimensional metal–organic framework
Room-temperature TRTS Fe3(THT)2(NH4)3 film sample · Thin Film · 800 nm pump at 80 uJ cm-2; about 1 THz probe bandwidth; complex conductivity at 0.3 ps after photoexcitation; nitrogen environment.
2018 · High-mobility band-like charge transport in a semiconducting two-dimensional metal–organic framework
High-mobility variable-temperature TRTS film · Thin Film · Complex photoconductivity measured at 0.3 ps after photoexcitation under vacuum from 300 K to 100 K.
No mapped measurement matches these filters.
These are the exact source-preserving method strings consolidated by this technique group.
| Raw method label | Mapped measurements |
|---|---|
| Frequency-resolved complex THz photoconductivity fitted by Drude-Smith model | 6 |
| Optical-pump terahertz-probe (OPTP) photoconductivity dynamics | 6 |
| Time-resolved terahertz spectroscopy (TRTS) | 4 |
| time-domain THz spectroscopy (THz-TDS), Drude-Smith fit | 4 |
| Optical pump-THz probe photoconductivity and Drude-Smith fit | 3 |
| Terahertz time-domain spectroscopy (THz-TDS) | 3 |
| Optical pump terahertz probe (OPTP) spectroscopy | 3 |
| optical pump terahertz probe (OPTP) | 3 |
| optical-pump terahertz-probe spectroscopy and Drude-Smith fitting | 3 |
| time-resolved terahertz spectroscopy with Drude-Smith fitting | 3 |
| optical-pump THz-probe spectroscopy (OPTP) | 3 |
| OPTP terahertz photoconductivity and Drude-Smith fit | 3 |
| Time-resolved terahertz spectroscopy and Drude-Smith fit | 2 |
| THz time-domain spectroscopy (THz-TDS) | 2 |
| time-resolved terahertz spectroscopy and Drude-Smith fitting | 2 |
| Optical-pump THz-probe frequency-resolved photoconductivity; Drude fit | 2 |
| Optical-pump THz-probe photoconductivity on powder films; Drude-Smith fit | 2 |
| Temperature-dependent frequency-resolved THz photoconductivity; Drude fit | 2 |
| Optical pump terahertz probe spectroscopy (OPTP) | 2 |
| optical-pump THz-probe spectroscopy with Drude-Smith fit | 2 |
| time-resolved terahertz spectroscopy (TRTS) | 2 |
| Time-resolved terahertz spectroscopy (optical pump-THz probe) | 1 |
| Variable-temperature TRTS with Drude fits | 1 |
| Time-domain terahertz spectroscopy (THz-TDS) | 1 |
| Terahertz time-domain spectroscopy with Drude-Smith fit | 1 |
| Temperature-dependent THz-TDS with Drude-Smith fits | 1 |
| Time-resolved terahertz spectroscopy (TRTS), fluence-dependent dynamics | 1 |
| Frequency-resolved complex TRTS with Drude/Drude-Smith fits | 1 |
| Temperature-dependent TRTS | 1 |
| steady-state THz spectroscopy and optical-pump THz-probe spectroscopy | 1 |
| optical-pump THz-probe spectroscopy and Drude fitting | 1 |
| temperature-dependent THz photoconductivity | 1 |
| steady-state ultrafast THz spectroscopy, frequency-resolved complex THz conductivity | 1 |
| time-resolved THz spectroscopy | 1 |
| Optical pump terahertz probe (OPTP) time-resolved photoconductivity | 1 |
| Time-resolved THz photoconductivity dynamics; biexponential fit | 1 |
| Post-TRTS pXRD | 1 |
| Optical-pump terahertz-probe (OPTP) transient photoconductivity | 1 |
| Time-resolved THz spectroscopy (TRTS) frequency-dependent photoconductivity | 1 |
| TRTS/OPTP pump-probe setup | 1 |
| THz-TDS refractive-index measurement | 1 |
| Spatially resolved THz-TDS transmission line scan | 1 |
| THz-TDS and TRTS after hydraulic pressing | 1 |
| THz-TDS | 1 |