Computational Modelling — Acid-Dependent Charge Transport in a Solution-Processed 2D Conductive Metal-Organic Framework

Measurement evidence

Computational Modelling

Acid-Dependent Charge Transport in a Solution-Processed 2D Conductive Metal-Organic Framework · Park G., Demuth M.C., Hendon C.H. et al. · Journal of the American Chemical Society · 2024

1 measurement group · 9 results

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

VASP 5.4.4 periodic DFT with PBEsol optimisation and HSEsol electronic structure; Gaussian09 NICS-xy

DFT model Cu3HHTATP2 · Model

Gamma-centred 1x1x3 k-mesh, 500 eV plane-wave cutoff, ionic convergence 0.005 eV A^-1, electronic convergence 10^-5 eV.

Geometry
monolayer, bulk, bilayer, linker NICS-xy and protonation-state models
Context
model systems for Cu3HHTATP2 and Cu3HHTP2
Measurement source
S8-S9 · DFT calculations · Figures 3, S3, S8
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
DFT-computed bulk in-plane electronic gap0.51 eVText
Exact Reported
11495 · Results and Discussion · Figure 3
Relative energy of 1122 ligand configuration+4.2 kcal/molFigure Axis
Rounded Reported
S11 · Figure S3 · Figure S3c
Relative energy of 1212 ligand configuration+18.8 kcal/molFigure Axis
Rounded Reported
S11 · Figure S3 · Figure S3c
Relative energy of 1221 ligand configuration+7.5 kcal/molFigure Axis
Rounded Reported
S11 · Figure S3 · Figure S3c
DFT-predicted interlayer spacing0.334 nmText
Exact Reported
11495 · Results and Discussion · Figure S8
DFT-predicted in-plane lattice parameter1.87 nmText
Exact Reported
11495 · Results and Discussion · Figure S8
DFT-predicted out-of-plane metallicitybulk structure features out-of-plane metallicity in eclipsed configurationCaption
Qualitative
11495 · Figure 3 caption · Figure 3
Monolayer Cu3HHTATP2 work functionPhi = 4.2 eVFigure Axis
Rounded Reported
11495 · Figure 3 · Figure 3
Monolayer Cu3HHTP2 work functionPhi = 5.0 eVFigure Axis
Rounded Reported
11495 · Figure 3 · Figure 3