Electrical Transport — The Growth Mechanism of a Conductive MOF Thin Film in Spray-based Layer-by-layer Liquid Phase Epitaxy

Measurement evidence

Electrical Transport

The Growth Mechanism of a Conductive MOF Thin Film in Spray-based Layer-by-layer Liquid Phase Epitaxy · Zheng R., Fu Z.-H., Deng W.-H. et al. · Angewandte Chemie - International Edition · 2022 · e202212797

3 measurement groups · 11 results

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

AC complex impedance spectroscopy / EIS Nyquist analysis

Cu3(HHTP)2-xC spray LBL-LPE thin-film growth-cycle series, x = 1-60 · Thin Film

Cu3(HHTP)2-xC films x = 5, 10, 15, 20, 30, 40, 50 and 60; Solartron SI 1260 impedance/gain phase analyser; gold wire 50 um; quasi-quad probe at room temperature; 300 mV AC amplitude; 10^-1 to 10^6 Hz; ZView2 equivalent-circuit fitting.

Temperature
room temperature
Atmosphere
not specified
Geometry
device dimension as in Figure 2d, Cr/Au electrodes with 10 um channel width
Context
pristine Cu3(HHTP)2-xC thin-film series
Measurement source
p004-p005 · 1.5 Evaluation of AC complex impedance spectra · Figure 3a-b; Figure S8
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
early-cycle bulk resistance dominanceat first 5 cycles, Rb is approximately 10 times higher than Rgb and RcapproximatelyText
Approximate
p004 · Results and Discussion · Figure 3b
AC impedance frequency range10^-1 to 10^6 HzText
Range
p003 · Results and Discussion · Figure 3a
Nyquist semicircle and resistance trend with growth cyclesemicircle diameter decreases with growth cycle; Rb and Rgb decrease with a power-function model rather than a linear modelText
Qualitative
p003 · Results and Discussion · Figure 3a-b; Figure S8
resistance-change saturation cycledecrease of Rb, Rgb and Rc slows and approaches saturation after the 10th growth cycleafter the 10th growth cycleText
Rounded Reported
p004 · Results and Discussion · Figure 3b inset

two-contact probe conductivity

HHTP powder pellet · Pellet

HHTP powder pellet measured by the same Keithley 4200 two-contact probe method at room temperature.

Temperature
room temperature
Atmosphere
ambient/not specified
Geometry
powder pellet; exact dimensions not reported
Context
non-MOF ligand control
Measurement source
p004 · 1.4 Evaluation of Electronic Conductivity · Figure S3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
HHTP pellet conductivity3.4 x 10^-9 S cm^-13.4e-7 S m^-1error bar shown, numeric uncertainty not labelledFigure Axis
Approximate
p007 · 2. Figures · Figure S3

two-contact probe DC I-V conductivity

Cu3(HHTP)2-xC spray LBL-LPE thin-film growth-cycle series, x = 1-60 · Thin Film

Keithley 4200 semiconductor analysis system at room temperature; applied voltage -5 to 5 V with 0.1 V scan step; conductivity calculated as sigma = thickness/(A.R).

Temperature
room temperature
Atmosphere
ambient/not specified
Geometry
Cr/Au electrodes on sapphire; Figure 2d shows 1000 um electrode length and 10 um channel width / MOF film gap
Context
pristine Cu3(HHTP)2-xC thin-film series; HHTP pellet control also measured
Measurement source
p004 · 1.4 Evaluation of Electronic Conductivity · Figure 2d-f; Figure S6
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Cu3(HHTP)2-20C conductivity from SI comparisonMarked as a best value within this paper1.4 x 10^-2 S cm^-11.4 S m^-1error bar shown, numeric uncertainty not labelledFigure Axis
Approximate
p007 · 2. Figures · Figure S3
10-cycle conductivity after rapid rise2.1 x 10^-3 S cm^-10.21 S m^-1Text
Rounded Reported
p003 · Results and Discussion · Figure 2f
conductivity increase over first 10 growth cyclesfrom 3.8 x 10^-7 to 2.1 x 10^-3 S cm^-1, about 5500 timesapproximately 5500 timesText
Rounded Reported
p003 · Results and Discussion · Figure 2f
low-cycle conductivity start point3.8 x 10^-7 S cm^-10.000038 S m^-1Text
Rounded Reported
p003 · Results and Discussion · Figure 2f
Cu3(HHTP)2-1C I-V behaviournonlinear I-V curve and very low currentText
Qualitative
p003 · Results and Discussion · Figure S6b
Cu3(HHTP)2-3C I-V behaviourgood linearity of I-V curve; uniform and continuous thin filmText
Qualitative
p003 · Results and Discussion · Figure S6d