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Published 2024 | Version v1
Journal article

A comprehensive investigation of the structural, chemical, and dielectric properties of co-doped YMnO3 multiferroic component

  • 1. Tallinn European School, Tehnika 18, 10149, Tallinn (Estonia)
  • 2. CEITEC BUT, Brno University of Technology, Purkyňova 123, 612 00, Brno (Czech Republic)
  • 3. Istanbul Medeniyet University Science and Advanced Technology Research Center (IMU-BILTAM), Istanbul (Turkey)
  • 4. Faculty of Engineering and Natural Sciences, Department of Engineering Physics, Istanbul Medeniyet University, Uskudar, 34700, Istanbul (Turkey)
  • 5. Faculty of Engineering and Natural Sciences, Department of Mechanical Engineering, Istanbul Bilgi University, Eyüpsultan, 34060, Istanbul (Turkey)
  • 6. Department of Biomedical Engineering, Faculty of Engineering and Natural Sciences, Biruni University, 34015, Istanbul (Turkey)
  • 7. Department of Physics, Lamar University, 77710, Beaumont, TX (United States)
  • 8. Faculty of Science, Department of Physics, Eskisehir Technical University, Yunusemre Campus, Eskisehir (Turkey)

Description

The solid-state reaction technique was employed to synthesize compounds of YMnO3 (YMO) and YMn1xCoxO3 (YMCO) with various Co doping levels (x = 0.01, 0.10, 0.20, and 0.40), where Co atoms partially substituted Mn sites. XRD studies confirmed the presence of two phases, YMO and Y0.98CoO3 (YCO), for doping ratios above x = 0.10. Additionally, an increase in crystalline size was observed with cobalt substitution. Surface characteristics of synthesized pellets were examined using scanning electron microscopy (SEM), revealing a less porous structure with cobalt doping. XPS analysis elucidated valence states, showing the presence of both Mn3+ and Mn4+, as well as Co2+ and Co3+. The x = 0.20 and 0.40 Co-doped samples exhibited lower grain and grain boundary energies compared to other samples, such as a decrease from 0.556 eV (undoped) to 0.195 eV (x = 0.20). Moreover, the dielectric constants of x = 0.20 and 0.40 cobalt-doped samples (around 320) significantly surpassed the undoped sample (around 22) at 106 Hz and 100 °C. The x = 0.20 cobalt-doped sample demonstrated the highest conductivity at 100 °C and 106 Hz (31 × 104 S/cm). FT-IR analysis provided insights into vibration and bending modes, and frequency- and temperature-dependent electrical features were investigated. It was observed that a single conduction model is insufficient to fully explain the conduction mechanism in these samples.

Additional details

Identifiers

Publishing Information

Journal Title
Applied Physics. A, Materials Science and Processing (Print)
Journal Volume
130
Journal Issue
3
Journal Page Range
vp.
ISSN
0947-8396
CODEN
APAMFC

Optional Information

Notes
AID: 166