Published November 25, 2015 | Version v1
Journal article

Influence of the oxygen pressure on the preferred orientation and optical properties of the pulsed-laser deposited Mn1.56Co0.96Ni0.48O4±δ thin films

  • 1. University of Chinese Academy of Sciences, Beijing 100049 (China)
  • 2. Key Laboratory of Functional Materials and Devices for Special Environments of CAS, Xinjiang Key Laboratory of Electronic Information Materials and Devices, Xinjiang Technical Institute of Physics & Chemistry of CAS, Urumqi 830011 (China)
  • 3. Key Laboratory of Nanodevices and Applications, Suzhou Institute of Nano-Tech and Nano-Bionics of CAS, Suzhou 215123 (China)

Description

Mn1.56Co0.96Ni0.48O4±δ (MCN) thin films with different oxygen pressures (in the range of 2 × 10−4 to 2 Pa) are prepared on Si(100)/SiOx substrates by pulsed laser deposition technique. Effects of oxygen pressures on the microstructure and optical properties of the prepared thin films are investigated in detail. The grain sizes of films gradually decrease and the preferential orientation of the MCN films change from (400) to (113) as the oxygen pressure increases. The x-ray photoelectron spectroscopy results show that the composition of these films is proximity to that of the bulk material. In addition, the Mn3+/Mn4+ pairs increase with an increase in the oxygen pressures increase. From spectroscopic ellipsometer spectroscopy, it is found that both the refractive index n and extinction coefficient k of the (400)-oriented films have no obvious peaks, whereas in the (113)-oriented films, peaks are exist. This feature typically originates from a change in the crystal structure as oxygen pressures increase. Furthermore, the Raman active mode (around ca. 650 cm−1) of (400) films almost disappears, whilst the active mode in (113) films remain. - Highlights: • The Mn1.56Co0.96Ni0.48O4-δ (MCN) spinel films are deposited by pulsed laser deposition process at different oxygen pressures. • The preferential orientation of the films changes from (400) plane to (113) as the oxygen pressure increases. • The Eg of the (113) film is twice as large as that of the (400) film. • The Raman active mode (around ca. 650 cm−1) can be observed in the (113) films while not in the (400) film.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.jallcom.2015.07.257

Additional details

Identifiers

DOI
10.1016/j.jallcom.2015.07.257;
PII
S0925-8388(15)30655-1;

Publishing Information

Journal Title
Journal of Alloys and Compounds
Journal Volume
650
Journal Page Range
p. 305-310
ISSN
0925-8388
CODEN
JALCEU

Optional Information

Copyright
Copyright (c) 2015 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.