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. 2017 Dec 4;8:1916. doi: 10.1038/s41467-017-01727-6

Table 1.

Lattice match between Sn net planes of βSn and selected transition metal stannides

Phase Space group Pearson's symbol Lattice parameters (Å) Ref. Sn net plane δ <100>Sn (%) δ p (%)
a b c
Sn I4 1 /amd tI4 5.831 5.831 3.182 49 {100} <100>Sn
AuSn4 Aba2 oS20 6.512 6.516 11.707 50 (008) [100]AuSn4 11.7 9.4
PtSn 4 Ccca oS20 6.418 11.366 6.384 51 (080) [001]PtSn4 9.5 8.5
PdSn 4 Ccca oS20 6.442 11.445 6.389 46 (080) [001]PdSn4 9.6 8.3
αCoSn 3 Cmca oS32 16.864 6.268 6.270 52 (600) [010]αCoSn3 7.5 6.2
MnSn2 I4/mcm tI12 6.644 6.644 5.421 53 (001) <100>MnSn2 13.9 11.5
FeSn2 I4/mcm tI12 6.545 6.545 5.326 54 (001) <100>FeSn2 12.2 10.2
βIrSn 4 I4 1 /acd tI40 6.310 6.310 22.770 47 (0016) <100>βIrSn4 8.2 7.2
βCoSn 3 I4 1 /acd tI64 6.275 6.275 33.740 52 (0024) <100>βCoSn3 7.6 6.1

δ <100>Sn is the linear disregistry between <100>Sn and the parallel direction in each stannide

δ p is the planar disregistry defined in Eq. (1) and Fig. 2c. Phases with disregistries < 10% are typeset in bold