STRUCTURAL, MICROSTRUCTURAL AND ELECTRICAL PROPERTIES OF La0.67Ca0.33MnO3 FILMS DEPOSITED VIA PULSED LASER DEPOSITION

Authors

  • A. N. Ishak Superconductor and Thin Film Laboratory, Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia Author
  • Lik Nguong Lau Superconductor & Thin Films Laboratory, Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia Author
  • Kean Pah Lim Superconductor & Thin Films Laboratory, Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia Author
  • W. N. W. Wan Jusoh Superconductor & Thin Films Laboratory, Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia Author
  • Xiao Tong Hon Superconductor & Thin Films Laboratory, Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia Author
  • Y. J. Wong Superconductor & Thin Films Laboratory, Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia Author
  • Mohd Mustafa Awang Kechik Superconductor and Thin Films Laboratory, Department of Physics, Faculty of Science Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, Malaysia Author
  • Soo Kien Chen Superconductor and Thin Films Laboratory, Department of Physics, Faculty of Science Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, Malaysia Author
  • Abdul Halim Shaari Superconductor and Thin Films Laboratory, Department of Physics, Faculty of Science Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, Malaysia Author

Abstract

La0.67Ca0.33MnO3 films were prepared by pulsed laser deposition on single crystal MgO (100) glass substrates with different deposition times and post-annealed at 800 °C and 900 °C to study their influence on the physical properties. All samples showed orthorhombic crystal structure as observed from the X-ray diffraction analysis. LCMO films exhibited double phases (La0.67Ca0.33MnO3 and La0.15Ca0.85MnO3) when post-annealed at 800 °C attributed to the insufficient energy of LCMO particles in forming the single crystalline phase at lower temperature. As the samples were post-annealed at 900 °C, the particles obtained the optimise energy to re-crystalline and forms pure La0.67Ca0.33MnO3 phase. The formation of layer-by-layer structure accompany with some agglomerations of the grains have been observed in 800 °C of post-annealed samples. Meanwhile, irregular shape particles were obtained for samples that were post-annealed at 900 °C and some cauliflower-like structure can be seen at some part of the film. From electrical measurement, the highest value of TMI (metal-insulator transition) has been observed in LC-M10-8 sample (152 k). It is found that the lower the thickness of the film, the higher the TMI value due to less energy of electrons that pass through the grain boundaries thus resulting a lower resistivity.

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Published

24-02-2022