“…Desai et al demonstrated that In 2 Te 3 has two components, a low-temperature a-phase with regularly ordered vacancies and a high-temperature b-phase with fully disordered vacancies; the former transforms to the latter at about 893 K. 11 a-In 2 Te 3 has a facecentered cubic lattice with a = 1.850 nm, which is approximately three times the lattice parameter of b-In 2 Te 3 (a = 0.616 nm). On the other hand, it has been observed that Ga 2 Te 3 has a mesoscopic superstructured phase, having periodic vacancy planes, 12,13 as observed in Ga 2 Se 3 . 14 We hypothesized that, if we could create such vacancy planes in the bulk samples and control their size and periodicity, we could achieve a low j, due to the effective phonon scattering by the vacancy planes.…”