Computational Modelling — Ag Nanoparticles-Induced Metallic Conductivity in Thin Films of 2D Metal-Organic Framework Cu3(HHTP)2

Measurement evidence

Computational Modelling

Ag Nanoparticles-Induced Metallic Conductivity in Thin Films of 2D Metal-Organic Framework Cu3(HHTP)2 · Saha S., Ananthram K.S., Hassan N. et al. · Nano Letters · 2023 · 9326-9332

6 measurement groups · 35 results

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

Bader charge analysis using Henkelman's Group program

Cu3(HHTP)2/Ag interface DFT model · Model

Bader charge transfer across Cu3(HHTP)2/Ag interface and topmost layers

Geometry
periodic Ag interface model
Context
target interface model
Measurement source
S30-S32 · Supplementary Tables · Tables S1 and S3
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Cu3(HHTP)2/Ag atom-wise Ag effective Bader charge transfer-3.310015——SI Table
Exact Reported
S30 · Supplementary table · Supplementary Table 1
Cu3(HHTP)2/Ag atom-wise C effective Bader charge transfer1.634324——SI Table
Exact Reported
S30 · Supplementary table · Supplementary Table 1
Cu3(HHTP)2/Ag atom-wise Cu effective Bader charge transfer0.265757——SI Table
Exact Reported
S30 · Supplementary table · Supplementary Table 1
Cu3(HHTP)2/Ag atom-wise H effective Bader charge transfer0.333295——SI Table
Exact Reported
S30 · Supplementary table · Supplementary Table 1
Cu3(HHTP)2/Ag atom-wise O effective Bader charge transfer1.076653——SI Table
Exact Reported
S30 · Supplementary table · Supplementary Table 1
Cu3(HHTP)2/Ag topmost-layer Ag effective Bader charge transfer-3.110976——SI Table
Exact Reported
S32 · Supplementary table · Supplementary Table 3
Cu3(HHTP)2/Ag topmost-layer C effective Bader charge transfer1.459685——SI Table
Exact Reported
S32 · Supplementary table · Supplementary Table 3
Cu3(HHTP)2/Ag topmost-layer Cu effective Bader charge transfer0.235822——SI Table
Exact Reported
S32 · Supplementary table · Supplementary Table 3
Cu3(HHTP)2/Ag topmost-layer H effective Bader charge transfer0.223929——SI Table
Exact Reported
S32 · Supplementary table · Supplementary Table 3
Cu3(HHTP)2/Ag topmost-layer O effective Bader charge transfer0.925476——SI Table
Exact Reported
S32 · Supplementary table · Supplementary Table 3
Effective charge transfer from Ag to Cu3(HHTP)2 per interfacial unit cellMarked as a best value within this paper3.31 e——Text
Approximate
5 · DFT analysis · Tables S1-S4
Valence electrons contributing to Bader charge on Ag structure for Cu3(HHTP)2/Ag1485——Text
Exact Reported
S4 · Computational details
Valence electrons contributing to Bader charge on Cu3(HHTP)2 structure522——Text
Exact Reported
S4 · Computational details
Valence electrons contributing to Bader charge on Cu3(HHTP)2/Ag interface2007——Text
Exact Reported
S4 · Computational details

Bader charge analysis using Henkelman's Group program

CuTCNQ/Ag interface DFT model · Model

Bader charge transfer across CuTCNQ/Ag interface and topmost layers

Geometry
periodic Ag interface model
Context
AgNP comparator interface model
Measurement source
S31-S33 · Supplementary Tables · Tables S2 and S4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
CuTCNQ/Ag atom-wise Ag effective Bader charge transfer-2.650305——SI Table
Exact Reported
S31 · Supplementary table · Supplementary Table 2
CuTCNQ/Ag atom-wise C effective Bader charge transfer1.628377——SI Table
Exact Reported
S31 · Supplementary table · Supplementary Table 2
CuTCNQ/Ag atom-wise Cu effective Bader charge transfer0.138072——SI Table
Exact Reported
S31 · Supplementary table · Supplementary Table 2
CuTCNQ/Ag atom-wise H effective Bader charge transfer0.221663——SI Table
Exact Reported
S31 · Supplementary table · Supplementary Table 2
CuTCNQ/Ag atom-wise N effective Bader charge transfer0.662187——SI Table
Exact Reported
S31 · Supplementary table · Supplementary Table 2
CuTCNQ/Ag topmost-layer Ag effective Bader charge transfer-2.162873——SI Table
Exact Reported
S33 · Supplementary table · Supplementary Table 4
CuTCNQ/Ag topmost-layer C effective Bader charge transfer0.965125——SI Table
Exact Reported
S33 · Supplementary table · Supplementary Table 4
CuTCNQ/Ag topmost-layer Cu effective Bader charge transfer0.050927——SI Table
Exact Reported
S33 · Supplementary table · Supplementary Table 4
CuTCNQ/Ag topmost-layer H effective Bader charge transfer0.1307——SI Table
Exact Reported
S33 · Supplementary table · Supplementary Table 4
CuTCNQ/Ag topmost-layer N effective Bader charge transfer0.306095——SI Table
Exact Reported
S33 · Supplementary table · Supplementary Table 4
Effective charge transfer from Ag to CuTCNQ per interfacial unit cell2.65 e——Text
Approximate
5 · DFT analysis · Tables S1-S4
Valence electrons contributing to Bader charge on Ag structure for CuTCNQ/Ag957——Text
Exact Reported
S4 · Computational details
Valence electrons contributing to Bader charge on CuTCNQ structure664——Text
Exact Reported
S4 · Computational details
Valence electrons contributing to Bader charge on CuTCNQ/Ag interface1621——Text
Exact Reported
S4 · Computational details

DFT electronic-structure modelling with VASP, PAW method, PBE GGA functional; 3x3x1 Monkhorst-Pack grid for interface models

Pristine Cu3(HHTP)2 DFT model · Model

Calculated DOS of pristine Cu3(HHTP)2

Geometry
periodic model
Context
pristine model
Measurement source
4 · DFT analysis · Figure 5a
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Pristine Cu3(HHTP)2 DOS characternonzero DOS at EF with discontinuity between valence and conduction regions——Text
Qualitative
4 · DFT analysis · Figure 5a

DFT electronic-structure modelling with VASP, PAW method, PBE GGA functional; 3x3x1 Monkhorst-Pack grid for interface models

Cu3(HHTP)2/Ag interface DFT model · Model

Calculated DOS and charge density of Cu3(HHTP)2/Ag interface

Geometry
periodic Ag interface model
Context
target interface model
Measurement source
4 · DFT analysis · Figure 5b-c
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
New broad interfacial state energyaround ~2.4 eV close to CB minimum——Text
Approximate
4 · DFT analysis · Figure 5b
Cu3(HHTP)2/Ag DOS characterMarked as a best value within this paperdispersion of electronic density and continuous density of states——Text
Qualitative
4 · DFT analysis · Figure 5b
Monkhorst-Pack grid3x3x1——Text
Exact Reported
S4 · Computational details
Geometry optimisation force threshold0.01 eV/A——Text
Exact Reported
S4 · Computational details

DFT electronic-structure modelling with VASP, PAW method, PBE GGA functional; 3x3x1 Monkhorst-Pack grid for interface models

Pristine CuTCNQ DFT model · Model

Calculated DOS of pristine CuTCNQ

Geometry
periodic model
Context
pristine model
Measurement source
4 · DFT analysis · Figure S21
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Pristine CuTCNQ DOS charactertypical semiconducting system with finite density of states below EF——Text
Qualitative
4 · DFT analysis · Figure S21

DFT electronic-structure modelling with VASP, PAW method, PBE GGA functional; 3x3x1 Monkhorst-Pack grid for interface models

CuTCNQ/Ag interface DFT model · Model

Calculated DOS and charge density of CuTCNQ/Ag interface

Geometry
periodic Ag interface model
Context
AgNP comparator interface model
Measurement source
4 · DFT analysis · Figure S22
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
CuTCNQ/Ag DOS characterless pronounced dispersion across EF; slight shift of VB minimum across EF——Text
Qualitative
4 · DFT analysis · Figure S22