Two-contact bulk conductivity on pressed pellet
pressed Cu3(HHTN)2 pellet · Pellet
Pressed pellet measured from 298 to 385 K under constant 4.0 V bias; conductivity calculated using sigma = I L/(V A).
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| activation energy, low-temperature zone I | 827 meV | 0.827 eV | — | Text Exact Reported | 4 · 2.5 Electronic properties and tunability · Fig. 4c, Fig. S27 |
| bulk conductivity at 385 KMarked as a best value within this paper | 9.01 x 10^-8 S cm^-1 at 385 K | — | — | Text Exact Reported | 4 · 2.5 Electronic properties and tunability · Fig. 4b |
| thermal conductivity increase factor from 298 to 385 K | 94-fold increase within DeltaT of 87 K | — | — | Text Exact Reported | 4 · 2.5 Electronic properties and tunability · Fig. 4b |
| bulk conductivity at room temperature | 9.55 x 10^-10 S cm^-1 at room temperature | — | — | Text Exact Reported | 4 · 2.5 Electronic properties and tunability · Fig. 4b |
| constant voltage for pellet conductivity | 4.0 V | — | — | Text Exact Reported | 14 · S10 Measurement of Conductivity · Fig. S25 |
| thermal band gap, low-temperature zone I | 1.65 eV at 298-319 K | — | — | Text Exact Reported | 4 · 2.5 Electronic properties and tunability · Fig. 4c, Fig. S27 |
| thermal band gap, high-temperature zone IIMarked as a best value within this paper | 0.75 eV at 324-385 K | — | — | Text Exact Reported | 4 · 2.5 Electronic properties and tunability · Fig. 4c, Fig. S27 |