Copper Vacancies and Heavy Holes in the Two-Dimensional Semiconductor KCu 3– x Se 2
The two-dimensional material KCu 3–x Se 2 was synthesized using both a K 2 Se 3 flux and directly from the elements. It crystallizes in the CsAg 3 S 2 structure (monoclinic space group C2/m with a = 15.417(3) Å, b = 4.0742(8) Å, c = 8.3190(17) Å, and β = 112.94(3)°), and single-crystal refinement revealed infinite copper-deficient [Cu 3–x Se 2 ]– layers separated by K + ions. Thermal analysis indicated that KCu 3–x Se 2 melts congruently at ~755 °C. UV–vis spectroscopy showed an optical band gap of ~1.35 eV that is direct in nature, as confirmed by electronic structure calculations. Electronic transport measurements on single crystals yielded an in-plane resistivity of ~6 × 10 –1 Ω cm at 300 K that has a complex temperature dependence. The results of Seebeck coefficient measurements were consistent with a doped p-type semiconductor (S = +214 μV K –1 at 300 K), with doping being attributed to copper vacancies. Transport is dominated by low-mobility (on the order of 1 cm 2 V –1 s –1 ) holes caused by relatively flat valence bands with substantial Cu 3d character and a significant concentration of Cu ion vacancy defects (p ~ 10 19 cm –3 ) in this material. In conclusion, electronic band structure calculations showed that electrons should be significantly more mobile in this structure type.