Substitution
of Cd into the photovoltaic material Cu2ZnSnS4 has been previously shown to improve power conversion
efficiencies, and although various models for the structural disorder
have been proposed, full characterization of Cu2Zn1–x
Cd
x
SnS4 has been hampered by a lack of understanding about the local
structure around individual atoms. Through a combination of powder
X-ray diffraction and solid-state NMR spectroscopy (119Sn, 113Cd, 63Cu, and 67Zn), the
detailed structures of the entire series Cu2Zn1–x
Cd
x
SnS4 (x = 0–1), prepared as bulk samples by reaction of
the elements at 800 °C, have been examined. The ordered kesterite
structure in space group I4̅ of the end-member
Cu2ZnSnS4 (x = 0) was retained
up to Cu2Zn0.7Cd0.3SnS4 (x = 0.3) and the stannite structure in space group I4̅2m from Cu2Zn0.6Cd0.4SnS4 (x = 0.4) to the
end-member Cu2CdSnS4 (x = 1).
Although the structural transition at x = 0.4 was
confirmed, 113Cd NMR spectroscopy reveals the coexistence
of phases with I4̅ and I4̅2m structures in the intermediate region (x = 0.3–0.4), evidence for which was previously unattainable
from XRD data alone. The 119Sn NMR spectra indicated the
presence of Sn sites surrounded within distinct local chemical environments
imparted by the distribution of Zn and Cd atoms disordered within
the second coordination sphere, which could be resolved by their isotropic
chemical shifts and quantified by their peak areas. Ultrahigh-field
(21.1 T) 63Cu NMR spectroscopy revealed the two sets of
Cu sites in the I4̅ structure expected for
the lightly Cd-substituted members (up to Cu2Zn0.8Cd0.2SnS4) and one set of Cu sites in the I4̅2m structure for the more heavily
substituted members. The balance of evidence from the comparison of
experimental and DFT-computed 63Cu and 67Zn
NMR spectra suggests that Cu/Zn disorder does not occur. Instead,
Cd substitution in Cu2Zn1–x
Cd
x
SnS4 proceeds exclusively
through disorder of Zn and Cd atoms, at least in the bulk samples
examined.