Electrical Transport — Synthesis and structure of a non-van-der-Waals two-dimensional coordination polymer with superconductivity

Measurement evidence

Electrical Transport

Synthesis and structure of a non-van-der-Waals two-dimensional coordination polymer with superconductivity · Pan Z., Huang X., Fan Y. et al. · Nature Communications · 2024 · 9342

4 measurement groups · 12 results

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

Room-temperature two-probe and four-probe I-V measurement

Cu3BHT single-crystal four-probe device · Electrode

Out-of-plane I-V curves from Cu3BHT single-crystal device at room temperature.

Temperature
300
Geometry
Ti/Au electrodes perpendicular to crystal long axis; out-of-plane [001]/c-axis transport
Context
pristine single-crystal Cu3BHT device
Measurement source
3 · Single crystal device characterization · Figure 2b
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Room-temperature I-V contact behaviourlinear voltage-current behaviour; negligible two-probe/four-probe differenceQualitative
Qualitative
3 · Single crystal device characterization · Figure 2b

Magnetoresistance under applied magnetic field

Cu3BHT single-crystal four-probe device · Electrode

Resistance change measured at 1.7 K with magnetic field orientation aligned with the current direction; figure axis spans about -9 to +9 T.

Temperature
1.7
Geometry
Out-of-plane current direction in single-crystal device
Context
pristine single-crystal Cu3BHT device
Measurement source
4 · Single crystal device characterization · Figure 2e
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Positive magnetoresistance at 1.7 Kapproximately 2% increaseapproximatelyText
Approximate
4 · Single crystal device characterization · Figure 2e

Low-temperature four-contact superconductivity transport

Cu3BHT single-crystal four-probe device · Electrode

Quantum Design PPMS DynaCool with Electrical Transport Option; 0.05-1 K; magnetic field 0-1 T applied along ab plane and supercurrent along c-axis.

Temperature
0.05-1
Geometry
Custom four-contact probe cell, out-of-plane current
Context
pristine single-crystal Cu3BHT device
Measurement source
7 · Device fabrication / superconductivity · Figure 3d-f; Supplementary Fig. 20
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Superconducting coherence lengthMarked as a best value within this paper47 nmText
Rounded Reported
5 · Superconductivity characterization and magnetic properties · Figure 3f
Zero-temperature upper critical magnetic fieldMarked as a best value within this paper0.15 TText
Rounded Reported
5 · Superconductivity characterization and magnetic properties · Figure 3f
Superconducting transition temperatureMarked as a best value within this paper0.25 KText
Rounded Reported
5 · Superconductivity characterization and magnetic properties · Figure 3d
Field suppression of superconductivityAt a magnetic field of 1 T, superconductivity completely vanishesText
Rounded Reported
5 · Superconductivity characterization and magnetic properties · Figure 3e
Superconducting transition widthMarked as a best value within this paperDelta Tc of 40 mKText
Exact Reported
5 · Superconductivity characterization and magnetic properties · Figure 3d

Four-probe temperature-dependent resistivity and conductivity

Cu3BHT single-crystal four-probe device · Electrode

Variable-temperature single-crystal device measurements from 2 to 300 K using attoDRY 2100 with SR830 lock-in amplifier.

Temperature
2-300
Geometry
Four-probe out-of-plane single-crystal device
Context
pristine single-crystal Cu3BHT device
Measurement source
4 · Single crystal device characterization · Figure 2c,d; Supplementary Figs. 15-16
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Out-of-plane electrical conductivity at 2 KMarked as a best value within this paper10^4 S/cm at 2 KText
Rounded Reported
3 · Single crystal device characterization · Figure 2b,c
Out-of-plane electrical conductivity at 300 Kapproximately 10^3 S/cm at 300 KapproximatelyText
Approximate
3 · Single crystal device characterization · Figure 2b,c
Residual-resistance ratioMarked as a best value within this paperRRR value reaching up to 10up toText
Approximate
4 · Single crystal device characterization · Figure 2c
Linear resistivity regimerho proportional to T between 20 and 100 KText
Range
4 · Single crystal device characterization · Figure 2d
High-temperature resistivity power law exponentrho proportional to T^0.31 above 100 KText
Rounded Reported
4 · Single crystal device characterization · Figure 2d