One Structure, Two ElementsLuGe2 Superconductor vs Ordinary Metallic Conductor LuSn2.
A Case Study on How Site-Selective Germanium for Tin Atom Substitution
Leads to Modulating of the Charge Distribution
The substitution
of chemically similar elements in a given crystal structure is an
effective way to enhance physical properties, but the understanding
on such improvements is usually impeded because the substitutions
are random, and the roles of the different atoms cannot be distinguished
by crystallographic symmetry. Herein, we provide a detailed crystallographic
analysis and property measurements for the continuous solid solutions
LuGexSn2–x (0 < x < 2). The results show that
there is no apparent change of the global symmetry, with the end-members
LuGe2 and LuSn2, as well as the intermediate
LuGexSn2–x compositions adopting the ZrSi2 type structure
(space group Cmcm, Pearson index oC12). Yet, the refinements of the crystal structures from single-crystal
X-ray diffraction data show that Ge–Sn atom substitutions are
not random, but occur preferentially at the zigzag chain. The patterned
distribution of two group 14 elements leads to a significant variation
in chemical bonding and charge ordering within the other structural
fragment, the 2D square nets, thereby resulting in tuned electron
transport. The enhancement is greater than that for the typical Bloch–Gruneisen
model and more akin to that for the parallel-resistor model. Magnetization
measurements on single crystals show bulk superconductivity in all
LuGexSn2–x samples with shielding fractions as high as 90%. Specific
heat data confirm the effect to originate from residual metallic tin
in the material, indicating that Sn atom substitutions in the 2D square
nets cause disruptions of the hypervalent bonding and local anisotropy,
which ultimately leads to vanishing of the superconducting state in
the end-member LuGe2. This work sheds light on how the
complexity in chemical interactions by two different carbon congeners
leads to changes in the physical properties and how they can be correlated
with the induced charge distribution. These studies also provide a
general approach to modulation of charge density and. thus, of emerging
physical properties in other classes of intermetallic systems based
on the main-group elements of groups 13 to 15.