TY - JOUR
T1 - Structure evolution and entropy change of temperature and magnetic field induced magneto-structural transition in Mn1.1Fe0.9P 0.76Ge0.24
AU - Yue, Ming
AU - Liu, Danmin
AU - Huang, Qingzhen
AU - Wang, Tong
AU - Hu, Fengxia
AU - Li, Jingbo
AU - Rao, Guanghui
AU - Shen, Baogen
AU - Lynn, Jeffery W.
AU - Zhang, Jiuxing
PY - 2013/1/28
Y1 - 2013/1/28
N2 - The compound Mn1.1Fe0.9P0.76Ge 0.24 has been studied using neutron powder diffraction (NPD), differential scanning calorimeter (DSC), and magnetic measurements, in order to clarify the nature of the magnetic and structural transition and measure the associated entropy change (ΔS). The strongly first order transition occurs from a paramagnetic (PM) to a ferromagnetic (FM) phase and can be induced either by temperature or by an applied magnetic field. Our investigations indicate that the two processes exhibit identical evolutions regarding the crystal and magnetic structures, indicating they should have the same entropy change. We, therefore, conclude that the ΔSDSC obtained by the DSC method (where the transition is temperature induced) is valid also for the magnetically induced transition, thus avoiding uncertainties connected with the magnetic measurements. We have obtained the ΔSDSC = 33.8 J/kg · K for this sample upon cooling, which would increase to 42.7 J/kg · K for a impurity-free and completely homogeneous sample. For comparison, the magnetic entropy changes (ΔSM) induced by magnetic field and calculated using the Maxwell relation yields a ΔS M = 46.5J/kg · K, 38% higher than ΔSDSC. These entropy results are compared and discussed.
AB - The compound Mn1.1Fe0.9P0.76Ge 0.24 has been studied using neutron powder diffraction (NPD), differential scanning calorimeter (DSC), and magnetic measurements, in order to clarify the nature of the magnetic and structural transition and measure the associated entropy change (ΔS). The strongly first order transition occurs from a paramagnetic (PM) to a ferromagnetic (FM) phase and can be induced either by temperature or by an applied magnetic field. Our investigations indicate that the two processes exhibit identical evolutions regarding the crystal and magnetic structures, indicating they should have the same entropy change. We, therefore, conclude that the ΔSDSC obtained by the DSC method (where the transition is temperature induced) is valid also for the magnetically induced transition, thus avoiding uncertainties connected with the magnetic measurements. We have obtained the ΔSDSC = 33.8 J/kg · K for this sample upon cooling, which would increase to 42.7 J/kg · K for a impurity-free and completely homogeneous sample. For comparison, the magnetic entropy changes (ΔSM) induced by magnetic field and calculated using the Maxwell relation yields a ΔS M = 46.5J/kg · K, 38% higher than ΔSDSC. These entropy results are compared and discussed.
UR - https://www.scopus.com/pages/publications/84873667545
U2 - 10.1063/1.4788803
DO - 10.1063/1.4788803
M3 - Article
AN - SCOPUS:84873667545
SN - 0021-8979
VL - 113
JO - Journal of Applied Physics
JF - Journal of Applied Physics
IS - 4
M1 - 043925
ER -