Control of Columnar Grain Microstructure in CSD LaNiO<sub>3</sub> Films
Aleksandra V. Atanova,
Dmitry S. Seregin,
Olga M. Zhigalina,
Dmitry N. Khmelenin,
Georgy A. Orlov,
Daria I. Turkina,
Alexander S. Sigov,
Konstantin A. Vorotilov
Affiliations
Aleksandra V. Atanova
Shubnikov Institute of Crystallography of Federal Scientific Research Centre “Crystallography and Photonics”, Russian Academy of Sciences, 119333 Moscow, Russia
Dmitry S. Seregin
SEC “Technological Center”, MIREA—Russian Technological University (RTU MIREA), 119454 Moscow, Russia
Olga M. Zhigalina
Shubnikov Institute of Crystallography of Federal Scientific Research Centre “Crystallography and Photonics”, Russian Academy of Sciences, 119333 Moscow, Russia
Dmitry N. Khmelenin
Shubnikov Institute of Crystallography of Federal Scientific Research Centre “Crystallography and Photonics”, Russian Academy of Sciences, 119333 Moscow, Russia
Georgy A. Orlov
SEC “Technological Center”, MIREA—Russian Technological University (RTU MIREA), 119454 Moscow, Russia
Daria I. Turkina
Department of Materials and Technology, Bauman Moscow State Technical University, 105005 Moscow, Russia
Alexander S. Sigov
SEC “Technological Center”, MIREA—Russian Technological University (RTU MIREA), 119454 Moscow, Russia
Konstantin A. Vorotilov
SEC “Technological Center”, MIREA—Russian Technological University (RTU MIREA), 119454 Moscow, Russia
Conductive LaNiO3 (LNO) films with an ABO3 perovskite structure deposited on silicon wafers are a promising material for various electronics applications. The creation of a well-defined columnar grain structure in CSD (Chemical Solution Deposition) LNO films is challenging to achieve on an amorphous substrate. Here, we report the formation of columnar grain structure in LNO films deposited on the Si-SiO2 substrate via layer-by-layer deposition with the control of soft-baking temperature and high temperature annealing time of each deposited layer. The columnar structure is controlled not by typical heterogeneous nucleation on the film/substrate interface, but by the crystallites’ coalescence during the successive layers’ deposition and annealing. The columnar structure of LNO film provides the low resistivity value ρ~700 µOhm·cm and is well suited to lead zirconate-titanate (PZT) film growth with perfect crystalline structure and ferroelectric performance. These results extend the understanding of columnar grain growth via CSD techniques and may enable the development of new materials and devices for distinct applications.