. IntroductionThermoelectric (TE) materials have drawn increasing attention because of their potential applications in energy harvesting and electronic cooling devices. [ 1,2 ] The performance of a thermoelectric material is defi ned by its dimensionless fi gure of merit ZT = α 2 ( ρ κ ) −1 T , where α is the Seebeck coeffi cient (also called as thermopower), T is the absolute temperature, ρ is the electrical resistivity, and κ is the thermal conductivity. [ 3 ] Extensive research has been carried out attempting to discover thermoelectric materials with higher performance. [4][5][6][7][8][9][10] Among different types of TE materials, lead telluride (PbTe) has demonstrated a relatively high ZT value in the medium temperature region, which makes it a suitable material for power generation rather than cooling applications. [ 11 ] Many studies have been focused on the doping of PbTe alloys to optimize its carrier concentration, [ 12,13 ] manipulate its electronic density of states, [ 14 ] microstructure [ 15 ] as well as endotaxial nanostructure. [16][17][18] In 2004, Hsu et al. fi rst reported high ZT values of PbTe-based AgPb m SbTe m +2 alloys, which were abbreviated as LAST alloys by taking the names of constitutive elements. [ 19 ] The main contribution to the high ZT value in LAST alloys is their nanostructure feature with nanoscopic precipitates or nanodots with compositional fl uctuation, which reduces thermal conductivity due to enhanced phonon scattering but not greatly affects electrical conduction, owing to the endotaxial interface between the precipitates and the matrix. [ 19 ] In fact, our previous study revealed that thermal conductivity and electrical resistivity can be reduced at the same time by a traditional annealing treatment that facilitated the in-situ formation of precipitates of 5-20 nm in diameter. [ 20 ] A recent study has shown that optimization of hierarchical architecture from mesoscale grains and grain boundaries to nanoscale endotaxial precipitates is effective for further ZT enhancement. [ 21 ] This work recalled the importance of controlling grain-level microstructure, which can be easily realized in most thermoelectric materials. It is well known that refi ning microstructure by reducing grain sizes is a general approach to lowering the thermal conductivity. In fact, great ZT enhancement has been achieved in several kinds of thermoelectric alloys, and among them a good example is that signifi cant ZT elevation can be realized in half-Heusler alloys that have high thermal conductivity, which can be signifi cantly lowered by reducing grain sizes [ 22 ] or via a nanocomposite approach. [ 23 ] It was reported that grain refi nement could also lead to an increase in Seebeck coeffi cient in some thermoelectric materials due to an enhanced energy fi ltering effect at grain boundaries. [ 15,24 ] With a motivation to further increase the thermoelectric performance, a repeated mechanical alloying (MA)-spark plasma sintering (SPS) method was applied to the fabrication of LAST alloys and was in...