Computational Modelling — Dominant Role of Hole Transport Pathway in Achieving Record High Photoconductivity in Two-Dimensional Metal–Organic Frameworks

Measurement evidence

Computational Modelling

Dominant Role of Hole Transport Pathway in Achieving Record High Photoconductivity in Two-Dimensional Metal–Organic Frameworks · Wang D., Ostresh S., Streater D. et al. · Angewandte Chemie - International Edition · 2023 · e202309505

2 measurement groups · 15 results

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

DFT band structure and stacking calculations

Cu-HHTP DFT model · Model

VASP 6.2.1; PBE + D3BJ for stacking offsets; HSE06 screened hybrid for band energies; non-collinear spins and spin-orbit coupling included for Cu2+.

Geometry
model
Context
Cu-HHTP model
Measurement source
p005 · Results and Discussion · Figure 5; Figures S8-S10
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Cu band energetic isolationapprox 1.1 eVText
Approximate
p005 · Results and Discussion · Figure 5
flat Cu band above Fermi level2.5 eV above Fermi levelText
Approximate
p005 · Results and Discussion · Figure 5
Cu-HHTP band gap along ALHA0.13 eVText
Exact Reported
p005 · Results and Discussion · Figure 5
Cu-HHTP band gap along GMKG0.49 eVText
Exact Reported
p005 · Results and Discussion · Figure 5
Cu-HHTP band gap along KH0.08 eVText
Exact Reported
p005 · Results and Discussion · Figure 5
Cu-HHTP minimum band gap along ML0.07 eVText
Exact Reported
p005 · Results and Discussion · Figure 5
Cu-HHTP HHTP-to-Cu localised band gapapprox 0.4 eVText
Approximate
p005 · Results and Discussion · Figure 5
Cu-HHTP most stable xy offset(0 Angstrom, 2 Angstrom)Text
Exact Reported
p011 / SI p.S10 · S7 · Figure S8
400 nm excitation energy3.1 eVText
Rounded Reported
p005 · Results and Discussion · Figure 5
HHTP band above Fermi levelapprox 3.0 eV above Fermi levelText
Approximate
p005 · Results and Discussion · Figure 5
DFT fixed c-axis interlayer distance3.2 AngstromText
Exact Reported
p011 / SI p.S10 · S7
Cu-HHTP magnetic dipole x component at stable offset0.27Text
Exact Reported
p011 / SI p.S10 · S7 · Figure S10
Cu-HHTP magnetic dipole y component at stable offset-1.6Text
Exact Reported
p011 / SI p.S10 · S7 · Figure S10
Cu-HHTP magnetic dipole z component at stable offset-2.8Text
Exact Reported
p011 / SI p.S10 · S7 · Figure S10

DFT band structure and stacking calculations

Zn-HHTP DFT model · Model

Zn-HHTP stacking potential-energy surface and band structure compared with Cu-HHTP.

Geometry
model
Context
Zn-HHTP model
Measurement source
p011-p013 / SI p.S10-S12 · S7 · Figures S9 and S11
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Zn-HHTP HHTP-localised band gapapprox 2.1 eVText
Approximate
p005 · Results and Discussion · Figure S11