Low-temperature plasma enhanced atomic layer deposition of large area HfS_2 nanocrystal thin films

Hafnium disulfide(HfS2) is a promising two-dimensional material for scaling electronic devices due to its higher carrier mobility, in which the combination of two-dimensional materials with traditional semiconductors in the framework of CMOS-compatible technology is necessary. We reported on the deposition of HfS2 nanocrystals by remote plasma enhanced atomic layer deposition at low temperature using Hf(N(CH3)(C2H5))4 and H2S as the reaction precursors. Selflimiting reaction behavior was observed at the deposition temperatures ranging from 150℃ to 350℃, and the film thickness increased linearly with the growth cycles. The uniform HfS2 nanocrystal thin films were obtained with the size of nanocrystal grain up to 27 nm. It was demonstrated that higher deposition temperature could enlarge the grain size and improve the HfS2 crystallinity, while causing crystallization of the mixed HfO2 above 450℃. These results suggested that atomic layer deposition is a low-temperature route to synthesize high quality HfS2 nanocrystals for electronic device or electrochemical applications.     

Formation of high-Sn content polycrystalline GeSn films by pulsed laser annealing on co-sputtered amorphous GeSn on Ge substrate

Polycrystalline Ge_(1-x)Sn_x(poly-Ge_(1-x)Sn_x) alloy thin films with high Sn content( 10%) were fabricated by cosputtering amorphous GeSn(a-GeSn) on Ge(100) wafers and subsequently pulsed laser annealing with laser energy density in the range of 250 mJ/cm~2 to 550 mJ/cm~2. High quality poly-crystal Ge_(0.90) Sn_(0.10) and Ge_(0.82) Sn_(0.18) films with average grain sizes of 94 nm and 54 nm were obtained, respectively. Sn segregation at the grain boundaries makes Sn content in the poly-GeSn alloys slightly less than that in the corresponding primary a-GeSn. The crystalline grain size is reduced with the increase of the laser energy density or higher Sn content in the primary a-GeSn films due to the booming of nucleation numbers. The Raman peak shift of Ge-Ge mode in the poly crystalline GeSn can be attributed to Sn substitution, strain,and disorder. The dependence of Raman peak shift of the Ge-Ge mode caused by strain and disorder in GeSn films on full-width at half-maximum(FWHM) is well quantified by a linear relationship, which provides an effective method to evaluate the quality of poly-Ge_(1-x)Sn_x by Raman spectra.