SrSn3 was synthesized from the elements in a welded niobium ampoule. The cr
ystal structure was determined from X-ray single crystal data. Space group
R (3) over bar m, a = 6,940(2) Angstrom, c = 33,01(1) Angstrom, Z = 12, Pea
rson symbol hR48.
SrSn3 shows an ordered atomic distribution on four crystallographic sites.
The structure is build up from two closed packed atom layers (Sn1/Sr1 and S
n2/Sr2) each with the composition Sr:Sn = 1:3 and with hexagonal symmetry o
f the Sr atoms. The Sn atoms are shifted with respect to the ideal position
s of a closed packed layer in a way that Sn triangles, which are separated
by Sr atoms, result. Translational symmetry along the c axis arises from a
12-layer stacking sequence with hexagonal and cubic closest packing motives
. Due to the layer sequence ABABCACABCBC... units of three face-sharing Sn
octahedra result (condensation through Sn2 atoms) which form the Sn partial
structure. The octahedra chains run parallel to the c axis and are connect
ed by exclusively vertex sharing Sn octahedra (Sn1 atoms).
Temperature dependent susceptibility measurements reveal superconducting pr
operties. LMTO band structure calculations verify the metallic behavior. An
analysis of the density of states with the help of the electron localizati
on function (ELF) shows, that two kinds of lone pairs occur in this interme
tallic phase: non-bonding electron pairs with the shape of a sp(2) orbital
hybrid are located at the Sn2 atoms and lone pairs with p orbital character
are located at Sn1 atoms. The role of lone pairs with respect to the super
conducting property is discussed.