Electrical Transport — Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers

Measurement evidence

Electrical Transport

Exceptionally high charge mobility in phthalocyanine-based poly(benzimidazobenzophenanthroline)-ladder-type two-dimensional conjugated polymers · Wang M., Fu S., Petkov P. et al. · Nature Materials · 2023 · 880-887

7 measurement groups · 22 results

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

Optical-pump THz-probe frequency-resolved photoconductivity; Drude fit

2DCP-CuPc thin film on fused silica · Thin Film

800 nm/1.55 eV optical excitation; dry N2 transmission geometry; room temperature.

Temperature
298
Atmosphere
dry N2
Geometry
thin film on fused silica
Context
pristine
Measurement source
884 · Frequency-resolved THz photoconductivity measurements · Fig. 5a,b; Supplementary Table 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-CuPc diffusion length~157 nmText
Approximate
884-885 · Frequency-resolved THz photoconductivity measurements
2DCP-CuPc room-temperature THz charge mobility460 +/- 31 cm2 V-1 s-1+/- 31 cm2 V-1 s-1SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-CuPc room-temperature Drude scattering time45 +/- 3 fs+/- 3 fsSI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4

Optical-pump THz-probe photoconductivity on powder films; Drude-Smith fit

2DCP-CuPc powder · Powder

Powder sandwiched between two fused silica substrates to form tens-of-micrometre films.

Temperature
298
Geometry
powder between fused silica substrates
Context
pristine
Measurement source
S54-S56 · Supplementary Figure 62 · Supplementary Fig. 62; Supplementary Table 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-CuPc powder Drude-Smith c parameter-0.74 +/- 0.02+/- 0.02SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-CuPc powder THz charge mobility183 +/- 19 cm2 V-1 s-1+/- 19 cm2 V-1 s-1SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-CuPc powder Drude-Smith scattering time69 +/- 7 fs+/- 7 fsSI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4

Optical-pump THz-probe frequency-resolved photoconductivity; Drude fit

2DCP-NiPc thin film on fused silica · Thin Film

800 nm/1.55 eV optical excitation; dry N2 transmission geometry; room temperature.

Temperature
298
Atmosphere
dry N2
Geometry
thin film on fused silica
Context
pristine
Measurement source
884 · Frequency-resolved THz photoconductivity measurements · Fig. 5a,b; Supplementary Table 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-NiPc diffusion lengthMarked as a best value within this paper~237 nmText
Approximate
884-885 · Frequency-resolved THz photoconductivity measurements
2DCP-NiPc room-temperature THz charge mobilityMarked as a best value within this paper971 +/- 44 cm2 V-1 s-1+/- 44 cm2 V-1 s-1SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-NiPc room-temperature Drude scattering time76 +/- 3 fs+/- 3 fsSI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4

Optical-pump THz-probe photoconductivity on powder films; Drude-Smith fit

2DCP-NiPc powder · Powder

Powder sandwiched between two fused silica substrates to form tens-of-micrometre films.

Temperature
298
Geometry
powder between fused silica substrates
Context
pristine
Measurement source
S54-S56 · Supplementary Figure 62 · Supplementary Fig. 62; Supplementary Table 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-NiPc powder Drude-Smith c parameter-0.72 +/- 0.01+/- 0.01SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-NiPc powder THz charge mobility219 +/- 14 cm2 V-1 s-1+/- 14 cm2 V-1 s-1SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-NiPc powder Drude-Smith scattering time61 +/- 4 fs+/- 4 fsSI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4

Temperature-dependent frequency-resolved THz photoconductivity; Drude fit

2DCP-CuPc thin film on fused silica · Thin Film

Cryostat under vacuum; 298 K to 78 K.

Temperature
78-298
Atmosphere
vacuum, pressure < 2e-4 mbar
Geometry
thin film on fused silica
Context
pristine
Measurement source
885 · Discussion · Fig. 5d; Supplementary Table 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-CuPc THz charge mobility at 78 K706 +/- 37 cm2 V-1 s-1+/- 37 cm2 V-1 s-1SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-CuPc Drude scattering time at 78 K69 +/- 4 fs+/- 4 fsSI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4

Temperature-dependent frequency-resolved THz photoconductivity; Drude fit

2DCP-NiPc thin film on fused silica · Thin Film

Cryostat under vacuum; 298 K to 78 K.

Temperature
78-298
Atmosphere
vacuum, pressure < 2e-4 mbar
Geometry
thin film on fused silica
Context
pristine
Measurement source
885 · Discussion · Fig. 5c,d; Supplementary Figs. 63-65
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-NiPc THz charge mobility at 78 KMarked as a best value within this paper1386 +/- 96 cm2 V-1 s-1+/- 96 cm2 V-1 s-1SI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4
2DCP-NiPc Drude scattering time at 78 KMarked as a best value within this paper108 +/- 7 fs+/- 7 fsSI Table
Exact Reported
S62 · Supplementary Table 4 · Supplementary Table 4

Time-resolved THz photoconductivity dynamics; biexponential fit

2DCP-NiPc thin film on fused silica · Thin Film

1.55 eV pump excitation; photoconductivity decay fitted with two exponential components.

Temperature
298
Atmosphere
dry N2
Geometry
thin film on fused silica
Context
pristine
Measurement source
S61 · Supplementary Table 3 · Supplementary Table 3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2DCP-CuPc fast photoconductivity decay componentt1 = 4.5 psSI Table
Exact Reported
S61 · Supplementary Table 3 · Supplementary Table 3
2DCP-CuPc slow photoconductivity decay componentt2 = 34.3 psSI Table
Exact Reported
S61 · Supplementary Table 3 · Supplementary Table 3
2DCP-CuPc amplitude-weighted photoconductivity lifetimecalculated from A1=14.6, t1=4.5 ps, A2=17.8, t2=34.3 psCalculated From Reported
Rounded Reported
S61 · Supplementary Table 3 · Supplementary Table 3
2DCP-NiPc fast photoconductivity decay componentt1 = 4.5 psSI Table
Exact Reported
S61 · Supplementary Table 3 · Supplementary Table 3
2DCP-NiPc slow photoconductivity decay componentt2 = 40.5 psSI Table
Exact Reported
S61 · Supplementary Table 3 · Supplementary Table 3
2DCP-NiPc amplitude-weighted photoconductivity lifetimecalculated from A1=8.9, t1=4.5 ps, A2=9.0, t2=40.5 psCalculated From Reported
Rounded Reported
S61 · Supplementary Table 3 · Supplementary Table 3