Table 1 Summary of the obtained superconducting properties for YH6, CaH6, H3S, and D3S.

From: Full-bandwidth anisotropic Migdal-Eliashberg theory and its application to superhydrides

 

N(εF)[NH(εF)]

λ

\({\omega }_{\log }\)

TcmMc

TcUF

TcFSR

TcFBW

TcFBW+μ

Tc\({}^{\exp }\)

 

(eV−1)

 

(meV)

(K)

(K)

(K)

(K)

(K)

(K)

YH6

0.69 [0.32]

2.0

108

154

202

250

239

238

208–214

CaH6

0.31 [0.27]

2.0

104

148

188

205

200

198

~ 204

H3S

0.53 [0.27]

2.3

108

173

232

256

250

232

172–184

D3S

0.53 [0.27]

2.2

80

127

166

190

182

170

144–148

  1. The table lists the DOS N(εF) and the H partial DOS NH(εF) at the Fermi level, the electron-phonon coupling parameter λ, the logarithmic average of the phonon frequencies \({\omega }_{\log }\), and the superconducting critical temperature Tc according to the modified McMillan formula (mMc), the University of Florida machine-learning model (UF), the Fermi-surface-restricted approximation (FSR), and the full-bandwidth implementation without (FBW) and with (FBW+μ) the self-consistent chemical potential update scheme, and all experimental critical temperatures Tc\({}^{\exp }\) at 200 GPa available in the literature. The Tc\({}^{\exp }\) of Ref. 21 and Ref. 26 are used as reference for YH6 and CaH6, respectively; and the Tc\({}^{\exp }\) of Refs. 50,53,59 are used as reference for H3S and D3S.