Table 3 Comparison between theoretical \(\hbox {T}_c\) values reported by Szczesniak13, and \(\omega _{cp}\) and \(\hbox {N}_{{cp}}\) values obtained from \(D_{cp}(\omega ,T_c)\) functions calculated for \(\hbox {H}_3^{32}\hbox {S}\), \(\hbox {H}_3^{33}\hbox {S}\), \(\hbox {H}_3^{34}\hbox {S}\) and \(\hbox {H}_3^{36}\hbox {S}\) at 180 GPa.

From: Cooper-pair distribution function \(D_{cp}(\omega ,T_c)\) for superconducting \(\hbox {D}_3\hbox {S}\) and \(\hbox {H}_3\hbox {S}\)

\(\hbox {H}_3^{n}S\)

\(\hbox {T}_c\) [K]

\(\omega _{cp}\) [meV]

\(\hbox {N}_{{cp}}\) (\(\times 10^{-3}\))

\(\hbox {H}_3^{32}\hbox {S}\)

193.63

37.35

100.19

\(\hbox {H}_3^{33}\hbox {S}\)

209.00

36.90

164.23

\(\hbox {H}_3^{34}\hbox {S}\)

199.20

36.45

127.51

\(\hbox {H}_3^{36}\hbox {S}\)

193.91

35.55

114.82