Tin-Substituted Chalcopyrite: An n-Type Sulfide with Enhanced Thermoelectric Performance.

The dearth of n-type sulfides with thermoelectric performance comparable to that of their p-type analogues presents a problem in the fabrication of all-sulfide devices. Chalcopyrite (CuFeS2) offers a rare example of an n-type sulfide. Chemical substitution has been used to enhance the thermoelectric performance of chalcopyrite through preparation of Cu1-x Sn x FeS2 (0 ≤ x ≤ 0.1). Substitution induces a high level of mass and strain field fluctuation, leading to lattice softening and enhanced point-defect scattering. Together with dislocations and twinning identified by transmission electron microscopy, this provides a mechanism for scattering phonons with a wide range of mean free paths. Substituted materials retain a large density-of-states effective mass and, hence, a high Seebeck coefficient. Combined with a high charge-carrier mobility and, thus, high electrical conductivity, a 3-fold improvement in power factor is achieved. Density functional theory (DFT) calculations reveal that substitution leads to the creation of small polarons, involving localized Fe2+ states, as confirmed by X-ray photoelectron spectroscopy. Small polaron formation limits the increase in carrier concentration to values that are lower than expected on electron-counting grounds. An improved power factor, coupled with substantial reductions (up to 40%) in lattice thermal conductivity, increases the maximum figure-of-merit by 300%, to zT ≈ 0.3 at 673 K for Cu0.96Sn0.04FeS2.

Effect of Sn Substitution on the Thermoelectric Properties of Synthetic Tetrahedrite.

The present study reports the effect of Sn substitution on the structural and thermoelectric properties of synthetic tetrahedrite (Cu12Sb4S13) system. The samples were prepared with the intended compositions of Cu12Sb4- xSn xS13 ( x = 0.25, 0.35, 0.5, 1) and sintered using spark plasma sintering. A detailed structural characterization of the samples revealed tetrahedrite phase as the main phase with Sn substituting at both Cu and Sb sites instead of only Sb site. The theoretical calculations using density functional theory revealed that Sn at Cu(1) 12d or Cu(2) 12e site moves the Fermi level ( EF) toward the band gap, whereas Sn at Sb 8c site introduces hybridized hole states near EF. Consequently, a relatively high optimum power factor of 1.3 mW/mK2 was achieved by the x = 0.35 sample. The Sn-substituted samples exhibited a significant decrease in the total thermal conductivity (κT) compared to the pristine composition (Cu12Sb4S13), primarily because of reduced electronic thermal conductivity. Due to an optimum power factor (1.3 mW/mK2) and reduced thermal conductivity (0.9 W/mK), a maximum zT of 0.96 at 673 K was achieved for x = 0.35 sample, which is nearly 40% increment compared to that of the pristine (Cu12Sb4S13) sample.

Electronic and thermoelectric properties of Zn and Se double substituted tetrahedrite.

The influence of Zn and Se double substitution on the electronic and thermoelectric properties of tetrahedrite was investigated in this study. The samples Cu11Zn1Sb4S13-xSex (x = 0.25, 0.5, 0.75, 1, and 2) were prepared via solid state synthesis followed by field assisted sintering. The density functional theory (DFT) results showed that Se substitution introduces additional bands near the Fermi level (EF), with lower effective mass compared to Zn (only) substituted sample Cu11Zn1Sb4S13. Consequently, the electrical resistivity decreased with the increase in Se content which is attributed to the enhanced charge carrier mobility caused by the more dispersive Se states as indicated by DFT results. But the Seebeck coefficient was invariant with x, due to the enhancement of the density of states (DOS) at EF. The overall effect was an increase in power factor of the Cu11Zn1Sb4S13-xSex samples compared to Cu11Zn1Sb4S13. The Zn2+ substitution at the Cu1+ tetrahedral site resulted in a decrease of the carrier thermal conductivity due to the decrease in charge carrier concentration. Whereas Se substitution resulted in the decrease of lattice thermal conductivity due to additional phonon scattering caused by the S-Se mass difference. Simultaneous optimization of the power factor and thermal conductivity could thus be achieved via double substitution at Cu and S sites. A maximum thermoelectric figure of merit (zT) of 0.86 at 673 K was exhibited by the Cu11Zn1Sb4S12.75Se0.25 sample due to its relatively high power factor among the samples (0.9 mW m-1 K-2 at 673 K) coupled with very low total thermal conductivity (0.67 W m-1 K-1 at 673 K).