Computational Modelling — Turning 2D MOFs into Mixed Ionic-Electronic Conductors via Side Chain Engineering

Measurement evidence

Computational Modelling

Turning 2D MOFs into Mixed Ionic-Electronic Conductors via Side Chain Engineering · Roh H., Su A.Y., Oh C. et al. · Journal of the American Chemical Society · 2025 · 38419-38427

5 measurement groups · 10 results

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

Materials Studio Forcite UFF geometry optimisation

Ni-nOctyl computational model · Model

Universal force field, Ewald electrostatics, 0 GPa external pressure

Context
model system
Measurement source
p005 · Materials Studio · Figure 1 and Supplementary Figures 3-4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Ni-1EG Forcite c parameter4.166 ÅText
Exact Reported
p005 · Materials Studio · Figure 1 / Supplementary Figure 3
Ni-2EG Forcite c parameter4.183 ÅText
Exact Reported
p005 · Materials Studio · Figure 1 / Supplementary Figure 3
Ni-3EG Forcite c parameter4.289 ÅText
Exact Reported
p005 · Materials Studio · Figure 1 / Supplementary Figure 3
Ni-nBu Forcite c parameter4.331 ÅText
Exact Reported
p005 · Materials Studio · Figure 1 / Supplementary Figure 3
Ni-nOctyl Forcite c parameter4.406 ÅText
Exact Reported
p005 · Materials Studio · Figure 1 / Supplementary Figure 3

VASP DFT geometry optimisation and band structure

Cu-1EG computational model · Model

PAW/PBE, 520 eV cutoff, DFT-D3(BJ), full relaxation; k-path for P-62m

Context
model system
Measurement source
p005 · Computational Methods · Supplementary Table 5 / Figures 4, S34-S35
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
DFT-optimised c lattice parameterc = 3.919 ÅSI Table
Exact Reported
p026 · Supplementary Table 5 · Supplementary Table 5

VASP DFT geometry optimisation and band structure

Ni-1EG computational model · Model

PAW/PBE, 520 eV cutoff, DFT-D3(BJ), full relaxation; k-path for P-62m

Context
model system
Measurement source
p005 · Computational Methods · Supplementary Table 5 / Figures 4, S34-S35
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
calculated band gap range for 2D cMOFs0.30 to 0.43 eVText
Range
p007 · Results and Discussion · Figure 4
DFT-optimised c lattice parameterc = 4.0118 ÅSI Table
Exact Reported
p026 · Supplementary Table 5 · Supplementary Table 5

VASP DFT geometry optimisation and band structure

Ni-2EG computational model · Model

PAW/PBE, 520 eV cutoff, DFT-D3(BJ), full relaxation; k-path for P-62m

Context
model system
Measurement source
p005 · Computational Methods · Supplementary Table 5 / Figures 4, S34-S35
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
DFT-optimised c lattice parameterc = 4.0501 ÅSI Table
Exact Reported
p026 · Supplementary Table 5 · Supplementary Table 5

VASP DFT geometry optimisation and band structure

Ni-nBu computational model · Model

PAW/PBE, 520 eV cutoff, DFT-D3(BJ), full relaxation; k-path for P-62m

Context
model system
Measurement source
p005 · Computational Methods · Supplementary Table 5 / Figures 4, S34-S35
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
DFT-optimised c lattice parameterc = 4.1308 ÅSI Table
Exact Reported
p026 · Supplementary Table 5 · Supplementary Table 5