Electrical Transport — Cation-exchanged conductive Mn2DSBDC metal–organic frameworks: Synthesis, structure, and THz conductivity

Measurement evidence

Electrical Transport

Cation-exchanged conductive Mn2DSBDC metal–organic frameworks: Synthesis, structure, and THz conductivity · Pattengale B., Neu J., Tada A. et al. · Polyhedron · 2021 · 115182

4 measurement groups · 68 results

Reported values remain attached to the sample, method, conditions, extraction quality and source location that produced them.

time-domain THz spectroscopy (THz-TDS), Drude-Smith fit

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.

Geometry
pressed PTFE/MOF pellet
Context
pristine_or_exchanged_framework
Measurement source
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Figs. S5-S8; Table S3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Drude-Smith c parameter at 100 K-1.00(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 200 K-1.00(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 300 K-0.98(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 100 K2.00(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 200 K1.89(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 300 K1.88(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 100 K52(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 200 K45(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 300 K47(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 100 K2.1(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 200 K3.0(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 300 K2.9(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
real conductivity at ~1 THz, 100 K~22 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
real conductivity at ~1 THz, 200 K~24 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
real conductivity at ~1 THz, 300 K~23 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
representative spectroscopic AC conductivityapproximately 25 S/mText
Approximate
8 · 4 Conclusions · Fig. 6; Fig. S6
temperature dependence of THz conductivityno observable/significant temperature dependence from 100-300 KQualitative
Qualitative
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Fig. S5; Fig. S6

time-domain THz spectroscopy (THz-TDS), Drude-Smith fit

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.

Geometry
pressed PTFE/MOF pellet
Context
pristine_or_exchanged_framework
Measurement source
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Figs. S5-S8; Table S3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Drude-Smith c parameter at 100 K-0.99(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 200 K-0.96(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 300 K-0.98(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 100 K2.53(8)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 200 K2.70(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 300 K2.06(7)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 100 K40(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 200 K52(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 300 K39(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 100 K3.8(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 200 K2.7(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 300 K3.6(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
real conductivity at ~1 THz, 100 K~33 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
real conductivity at ~1 THz, 200 K~28 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
real conductivity at ~1 THz, 300 K~27 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
representative spectroscopic AC conductivityapproximately 25 S/mText
Approximate
8 · 4 Conclusions · Fig. 6; Fig. S6
temperature dependence of THz conductivityno observable/significant temperature dependence from 100-300 KQualitative
Qualitative
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Fig. S5; Fig. S6

time-domain THz spectroscopy (THz-TDS), Drude-Smith fit

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.

Geometry
pressed PTFE/MOF pellet
Context
pristine_or_exchanged_framework
Measurement source
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Figs. S5-S8; Table S3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Drude-Smith c parameter at 100 K-1.00(7)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 200 K-1.00(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 300 K-0.99(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 100 K1.55(7)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 200 K1.62(7)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 300 K1.710(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 100 K32(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 200 K36(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 300 K45(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 100 K4.6(6)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 200 K4.1(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 300 K3.2(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
real conductivity at ~1 THz, 100 K~28 S/m at ~1 THzFigure Axis
Approximate
7 · 3.3 / Supplementary Figures · Fig. 6a
real conductivity at ~1 THz, 200 K~30 S/m at ~1 THzFigure Axis
Approximate
7 · 3.3 / Supplementary Figures · Fig. 6a
real conductivity at ~1 THz, 300 K~25 S/m at ~1 THzFigure Axis
Approximate
7 · 3.3 / Supplementary Figures · Fig. 6a
representative spectroscopic AC conductivityapproximately 25 S/mText
Approximate
8 · 4 Conclusions · Fig. 6; Fig. S6
temperature dependence of THz conductivityno observable/significant temperature dependence from 100-300 KQualitative
Qualitative
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Fig. S5; Fig. S6

time-domain THz spectroscopy (THz-TDS), Drude-Smith fit

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.

Geometry
pressed PTFE/MOF pellet
Context
pristine_or_exchanged_framework
Measurement source
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Figs. S5-S8; Table S3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Drude-Smith c parameter at 100 K-0.98(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 200 K-0.97(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith c parameter at 300 K-0.93(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 100 K2.20(7)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 200 K2.20(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith lattice permittivity at 300 K2.20(2)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 100 K39(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 200 K38(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith scattering time τ at 300 K63(3)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 100 K3.6(5)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 200 K3.6(4)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
Drude-Smith plasma frequency ωp at 300 K2.4(1)SI Table
Exact Reported
S6 · Supplementary Tables · Table S3
real conductivity at ~1 THz, 100 K~36 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
real conductivity at ~1 THz, 200 K~31 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
real conductivity at ~1 THz, 300 K~34 S/m at ~1 THzFigure Axis
Approximate
S3-S4 · 3.3 / Supplementary Figures · Fig. S5/S6
representative spectroscopic AC conductivityapproximately 25 S/mText
Approximate
8 · 4 Conclusions · Fig. 6; Fig. S6
temperature dependence of THz conductivityno observable/significant temperature dependence from 100-300 KQualitative
Qualitative
7 · 3.3 Time domain THz spectroscopy · Fig. 6; Fig. S5; Fig. S6