Abstract
The dependence of magnetization M on temperature T and the applied magnetic field H were measured for the half-doping manganite Nd0.5Sr0.25Ca0.25MnO3. The M(T) curve exhibits that a paramagnetic (PM)–ferromagnetic (FM) phase transition occurs around 174 K. The PM–FM phase transition is considered to be a second-order phase transition due to the absence of hysteresis on its heating and cooling M(T) curves. Moreover, the second-order phase transition can be testified with the positive slope in Arrott plots. However, the scaling analysis of magnetic entropy change exhibits that ΔSM(T) curves do not collapse into a single universal curve, indicating that the observed PM–FM phase transition is not an authentic second-order phase transition. Due to the appearance of short-range FM coupling in PM region, the PM–FM phase transition at 225 K > T > 188 K is a first-order phase transition. The second-order phase transition only occurs at T < 188 K. When the magnetic field is increased above 1.5 T, the first-order phase transition can be converted into the second-order phase transition. The results shows that the magnetic entropy change scaling is an effective method to determine the nature of the PM–FM phase transition.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.