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The Research Of Magnetism And Magnetocaloric Effects In Rare Earth Transition Metal Oxides

Posted on:2024-05-20Degree:MasterType:Thesis
Country:ChinaCandidate:N Z HeFull Text:PDF
GTID:2542307103972629Subject:New generation electronic information technology (including quantum technology, etc.)
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Magnetic refrigeration technology based on the magnetocaloric effect(MCE)has been considered as one of the new solid refrigeration technologies,which can potentially replace the widely used gas compression refrigeration technology due to its advantages of green environmental protection,high efficiency and energy saving,stability,and reliability.The design and development of high-performance magnetic refrigeration materials is one of the key factors for the practical application of magnetic refrigeration technology.Recent studies have shown that some rare earth transition metal oxides have excellent magnetocaloric effect properties.Thus,in this paper,rare earth double perovskite oxides RE2CuTiO6(RE=Gd,Dy,Ho,Er),rare earth transition metal oxides Dy2BaCu1-xZnxO5(x=0.25,0.5,0.75)and Er2BaNi1-xTMxO5(x=0.33,0.67;TM=Cu,Zn)were studied as the research objects,and the magnetic phase transition types of rare earth transition metal oxide materials were adjusted by doping different transition metal elements,and the crystal structure,microstructure,magnetic phase transition,magnetic and magnetocaloric properties of the presentation materials were systematically studied.The main obtained findings are as follows:The investigation on the crystal structure of the rare earth double perovskite oxides RE2CuTiO6(RE=Gd,Dy,Ho,Er)illustrates that Gd2CuTiO6 oxide crystallizes in monoclinic crystal system(space group P21/c),whereas Dy2CuTiO6,Ho2CuTiO6,and Er2CuTiO6crystallize in hexagonal crystal system(space group P(?)2).RE2CuTiO6(RE=Gd,Dy,Ho,Er)oxides undergo a second-order magnetic phase transition from paramagnetic to ferromagnetic,and the magnetic phase transition temperatures are estimated to be 2.4 K,2.7 K,2.2 K,and 2.2 K,respectively.Under the applied magnetic field of 0-7 T,the maximum values of magnetic entropy change(-ΔSMmax)of Gd2CuTiO6,Dy2CuTiO6,Ho2CuTiO6,and Er2CuTiO6are 48.3,22.2,15.2,and 16.0 J/kg K,respectively.The values of temperature averaged entropy change[TEC(5 K)]are43.0,20.9,15.0,and 15.6 J/kg,respectively.The corresponding values of the relative cooling capacity(RCP)and refrigeration capacity(RC)are 477.0 and 359.2 J/kg,462.9and 354.9 J/kg,442.5 and 344.0,as well as 392.0 and 225.4 J/kg,respectively.The present results illustrate that RE2CuTiO6 oxides have excellent magnetocaloric properties in the low-temperature region,especially Gd2CuTiO6,which has great application potential in the field of low-temperature magnetic refrigeration.The crystal structure of Dy2BaCu1-xZnxO5(x=0.25,0.5,0.75)oxides belong to the orthogonal crystal with the space group Pnma.The magnetic measurement results show that Dy2BaCu0.75Zn0.25O5and Dy2BaCu0.5Zn0.5O5 undergo a first-order magnetic phase transition from paramagnetic to antiferromagnetic,while Dy2BaCu0.25Zn0.75O5 oxide undergoes a second order magnetic phase transition from paramagnetic to ferromagnetic.The magnetic phase transition temperatures are 12.1 K,9.8 K,and 2.1K for Dy2BaCu0.75Zn0.25O5,Dy2BaCu0.5Zn0.5O5,and Dy2BaCu0.25Zn0.75O5,respectively.With the increasing amount of Zn incorporation,Dy2BaCu1-xZnxO5(x=0.25,0.5,0.75)oxides will undergo the process from antiferromagnetic to ferromagnetic at low temperature,which is an effective method to adjust the magnetic phase transition of this series of oxides.Under the magnetic field of 0-7 T,the values of-ΔSMmaxand TEC(5K)are calculated to be 8.5 and 8.4 J/kg K,9.7 and 9.3 J/kg K,as well as 13.2 and 13.0J/kg K for Dy2BaCu0.75Zn0.25O5,Dy2BaCu0.5Zn0.5O5,and Dy2BaCu0.25Zn0.75O5,respectively.The corresponding values of RCP and RC are 227.4 and 178.0 J/kg,283.6and 213.6 J/kg,as well as 343.0 and 270.5 J/kg,respectively.The Er2BaNi1-xTMxO5(x=1/3,2/3;TM=Cu,Zn)oxides crystallize in the orthogonal crystal with space group Pnma that is different from the crystal structure of Er2BaNiO5,which indicates the doping of Cu and Zn elements can change the crystal structure.The magnetic measurement results show that all four oxides undergo a second-order magnetic phase transition from paramagnetic to ferromagnetic,among which the magnetic phase transition temperature of Er2BaNi0.67Cu0.33O5,Er2BaNi0.67Zn0.33O5,and Er2BaNi0.33Zn0.67O5oxides are all about 2.4 K,and the magnetic phase transition temperature of Er2BaNi0.33Cu0.67O5 oxide may be less than 2K.Under the magnetic field of 0-7 T,the values of-ΔSMmaxand TEC(5 K)are 7.8 and7.6 J/kg K,9.6 and 9.5 J/kg K,10.5 and 10.4 J/kg K,12.6 and 12.3 J/kg K for Er2BaNi0.67Cu0.33O5,Er2BaNi0.33Cu0.67O5,Er2BaNi0.67Zn0.33O5,and Er2BaNi0.33Zn0.67O5,respectively.Accordingly,the values of RCP and RC are 251.9 and 199.8 J/kg,266.3and 206.0 J/kg,respectively.276.5 and 215.7 J/kg,268.7 and 207.0 J/kg,respectively.
Keywords/Search Tags:Rare-earth transition metal oxides, Double perovskite oxides, Magnetism, Magnetic phase transition, Magnetocaloric effect
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