Table 2 Promising TCMs from HT calculations
From: Transparent conducting materials discovery using high-throughput computing
Peng et al.35 | \({\boldsymbol{E}}_{\boldsymbol{g}}^{{\boldsymbol{GW}}}\) (eV) | \({\boldsymbol{M}}_{{\mathbf{DOS}}}^ \ast\) |
|---|---|---|
Cr2MnO4 | 3.3 | 9.8 |
Hautier et al.24 | \({\boldsymbol{E}}_{\boldsymbol{g}}^{{\boldsymbol{GW}}}\) (eV) | \({\boldsymbol{M}}_{\boldsymbol{\sigma }}^ \ast\) |
K2Sn2O3 | 2.3 | 0.27 |
Rb2Sn2O3 | 2.3 | 0.37 |
K2Pb2O3 | 2.6 | 0.39 |
K2Sn2O3 | 2.4 | 0.42 |
Sb4Cl2O5 | 3.8 | 0.49 |
PbTiO3 | 3.2 | 0.48 |
B6O | 3.0 | 0.71 |
Ca4As2O | 2.1 | 0.76 |
PbHfO3 | 3.5 | 1.08 |
PbTiO3 | 3.7 | 1.09 |
PbZrO3 | 3.6 | 1.09 |
Tl4O3 | 1.6 | 1.16 |
Ca4P2O | 2.3 | 1.19 |
ZrSO | 4.3 | 1.25 |
HfSO | 4.5 | 1.30 |
NaNbO2 | 2.1 | 1.36 |
Sr4P2O | 2.4 | 1.36 |
Hg2SO4 | 3.8 | 1.37 |
Tl4V2O7 | 4.5 | 1.44 |
Sr4As2O | 2.2 | 1.46 |
Hautier et al. 28 | Eg (eV) | \(M^{e^\ast} _\sigma\) |
Cd2Ge7O16 | 4.9 (exp.) | 0.16 |
CdGeO3 | 2.4 (GW) | 0.18 |
In6TeO12 | 1.7 (GW) | 0.18 |
Cd2Sb2O7 | 2.8 (exp.) | 0.19 |
HgAs2O6 | 1 (GW) | 0.19 |
HgAsO3 | 2.4 (GW) | 0.20 |
Cd3Cl2O2 | 1.7 (GW) | 0.21 |
ZnSb2O6 | 3 (exp.) | 0.21 |
In2TeO6 | 2.0 (GW) | 0.21 |
GeO2 | >4 (exp.) | 0.22 |
Cd2GeO4 | 3.2 (exp.) | 0.22 |
Ga2TeO6 | 2.2 (GW) | 0.22 |
Bhatia et al. 103 | \(E_g^{GW}\) (eV) | \(M_\sigma ^ \ast\) |
Ba2BiTaO6 | 3.8 | 0.45 |
Sarmadian et al. 30 | \(E_g^{{\mathrm{HSE}}}\) (eV) | \(M_{{\mathrm{line}}}^ \ast\) |
Pr2SeO2 | 3.26 | 0.69 |
Gd2SeO2 | 3.07 | 0.76 |
Nd2SeO2 | 2.76 | 0.79 |
La2SeO2 | 3.49 | 0.92 |
Cerqueira et al. 106 | \(E_g^{{\mathrm{DFT}}}\) (eV) | \(M_\sigma ^ \ast\) |
AuFeO2 | 0.6 | 0.59 |
AuScO2 | 1.8 | 0.63 |
AuAlO2 | 0.6 | 0.71 |
AgFeO2 | 1.1 | 0.90 |
AuCoO2 | 0.5 | 1.03 |
AgGaO2 | 0.6 | 1.09 |
AgSrO2 | 0.6 | 1.27 |
AuBaO2 | 1.2 | 1.44 |
AgAlO2 | 1.4 | 1.49 |
AuBiO2 | 1.3 | 1.54 |
AgBO2 | 1.4 | 1.61 |
AuCrO2 | 1.2 | 1.65 |
AuHO2 | 0.7 | 1.68 |
AuCdO2 | 0.9 | 1.76 |
AgAuO2 | 0.6 | 1.80 |
AuSrO2 | 1.3 | 1.80 |
AgLiO2 | 0.5 | 1.85 |
CuFeO2 | 0.9 | 2.02 |
AgRhO2 | 0.5 | 2.14 |
CuHO2 | 0.5 | 2.23 |
CuGaO2 | 0.8 | 2.23 |
CuBiO2 | 1.0 | 2.29 |
AgBiO2 | 1.4 | 2.38 |
AgCrO2 | 1.7 | 2.48 |
AuYO2 | 2.7 | 2.49 |
AgNO2 | 1.4 | 2.57 |
AgScO2 | 2.1 | 2.58 |
CuRhO2 | 0.7 | 2.75 |
Shi et al. 107 | \(E_g^{{\mathrm{HSE}}}\) (eV) | \(M_\sigma ^ \ast\) |
AgYS2 | 3.16 | 0.71 |
KYS2 | 3.37 | 1.23 |
CsLaO2 | 4.11 | 2.16 |
BrLaO2 | 3.92 | 2.23 |
Yim et al. 37 | \(E_g^{\mathrm{HSE}}\) (eV) | \(M_{{\mathrm{line}}}^ \ast\) |
Rb2Sn2O3 | 0.28 | 1.66 |
La4O4Se3 | 0.29 | 1.68 |
K2Sn2O3 | 0.32 | 1.89 |
Cu3VO4 | 2.55 | 2.01 |
CsCuO | 1.21 | 2.45 |
Cu3PO4 | 3.50 | 2.55 |
BaCu2O2 | 2.34 | 2.75 |
Cu2LiO2 | 2.06 | 2.79 |
CuRbO | 6.02 | 2.80 |
Cu2NaO2 | 2.19 | 2.83 |
CuNaO | 9.01 | 2.96 |
CuKO | 5.73 | 2.99 |
Sn4O2F4 | 1.68 | 3.05 |
CuLiO | 2.76 | 3.10 |
La2O2Te | 0.65 | 3.12 |
Cu2SO4 | 3.78 | 3.19 |
Y2OS2 | 1.41 | 3.67 |
SnSO4 | 1.12 | 5.40 |
Yan et al. 105 | \(E_g^{{\mathrm{HSE}} + {\mathrm{GW}}}\) (eV) | \(M_{{\mathrm{fitted}}}^ \ast\) |
TaIrGe | 2.64 | 0.39–0.96 |
Varley et al. 108 | \(E_g^{{\mathrm{DFT}}}\) (eV) | \(m_\sigma ^ \ast\) |
BP | 1.24 | 0.34 |
AlP | 1.63 | 0.56 |
Raghupathy et al. 29 | \(E_g^{{\mathrm{HSE}}}\) (eV) | \(M_{{\mathrm{fitted}}}^ \ast\) |
MgTe | 4.2 | 0.18 |
Al2Se3 | 3.1 | 0.56 |
ZnS | 3.5 | 0.70 |
MgS | 5.5 | 0.96 |
Raghupathy et al. 110 | \(E_g^{{\mathrm{HSE}}}\) (eV) | \(M_\sigma ^ \ast\) |
IrSbS | 3.08 | 0.39 |
Ba2GeSe4 | 3.01 | 0.60 |
Ba2SiSe4 | 3.96 | 0.75 |
Ba(BSe3)2 | 3.53 | 0.78 |
NbCu3Se4 | 3.13 | 0.82 |
VCu3S4 | 3.68 | 0.93 |
CuBS2 | 3.41 | 1.00 |
Ha et al. 109 | \(E_g^{GW} (eV)\) | \(M^\ast_\sigma\) |
Li3Sb | 3.06 | 0.24 |
CaTe | 3.50 | 0.60 |