Gotowa bibliografia na temat „R2NiMnO6”

AbstractThe crystal structure, cryogenic magnetic properties, and magnetocaloric performance of double perovskite Eu2NiMnO6 (ENMO), Gd2NiMnO6 (GNMO), and Tb2NiMnO6 (TNMO) ceramic powder samples synthesized by solid-state method have been investigated. X-ray diffraction structural investigation reveal that all compounds crystallize in the monoclinic structure with a P21/n space group. A ferromagnetic to paramagnetic (FM-PM) second-order phase transition occurred in ENMO, GNMO, and TNMO at 143, 130, and 112 K, respectively. Maximum magnetic entropy changes and relative cooling power with a 5 T applied magnetic field are determined to be 3.2, 3.8, 3.5 J/kgK and 150, 182, 176 J/kg for the investigated samples, respectively. The change in structural, magnetic, and magnetocaloric effect attributed to the superexchange mechanism of Ni2+–O–Mn3+ and Ni2+–O–Mn4+. The various atomic sizes of Eu, Gd, and Tb affect the ratio of Mn4+/Mn3+, which is responsible for the considerable change in properties of double perovskite.

Multifunctional materials with novel magnetic and electric properties have attracted intense research interest due to prospects in technological applications as well as understanding of fundamental physics. Perovskite materials with ABO3 structure belong to one of the most interesting and vastly studied families by virtue of their rich magnetic and electrical properties. In the present thesis, efforts have been made to investigate the magnetic, electrical, and structural properties of A and B-site doped perovskites. In the beginning, a general introduction to basic concepts of various physical phenomena are discussed. This is followed by a brief description of the various experimental methods employed including sample synthesis and single crystal growth. Fe3+ and Mn3+ have the same ionic radii in oxygen octahedra. However, Mn3+ is Jahn–Teller active, and the magnetic ground states of RFeO3 and RMnO3 are completely different. The evolution of structural and electrical properties with doping of Mn3+ ion in RFeO3 was investigated on a series of NdFe1-xMnxO3 (0≤x≤1) compounds. Despite similar ionic radii in Mn3+ and Fe3+, a large variation in the lattice parameters and a crossover from dynamic to static Jahn– Teller distortion were discernible. The magnitude of Fe/Mn–O–Fe/Mn bond angle on ab plane and activation energy corresponding to transport and dielectric relaxation (deduced by assuming the small polaron hopping (SPH) model) vary with doping in a characteristic manner which was attributed to changes in magnetic interaction. Effects of size mismatch at B-site were investigated by doping Mn-site with Ni cations in Ho2NiMnO6 compound. This induces B-site ordering which leads to double perovskite structure and ferromagnetic ordering at TC = 86 K. Ideal Curie–Weiss law fails to provide a reasonable fit in the paramagnetic region which follows a modified Curie–Weiss law. Such a deviation occurs due to presence of heavy rare earth element Ho. Griffiths phase pertaining to the Ni/Mn subsystem was ascertained. Two dielectric relaxations due to phononic and Maxwell–Wagner mechanisms were observed. The system has also been shown to be a potential magnetocaloric refrigerant. A solid solution of RFeO3 and RMnO3 offer much prospects due to its vastly different magnetic properties. A single crystalline phase is essential for such studies, and we were successful in growing single crystals of ErFe0.55Mn0.45O3 which order antiferromagnetically at 365 K with spin canting-induced weak ferromagnetic moment along c axis. Upon cooling, magnetization along c axis passes through zero at 266.4 K and becomes negative below this temperature and a spin reorientation occurs from Γ4(Gx, Ay, Fz) to Γ1(Ax, Gy, Cz) configuration in the temperature window of 255 to 258 K. Magnetic behavior is explained with spin configuration and interplay between net magnetization of individual Er and Fe/Mn sublattices which are oppositely coupled and have different temperature evolution. To observe the effect of A-site doping on RFeO3 perovskites, Ho0.5Dy0.5FeO3 single crystals were grown. Two spin reorientations of Fe magnetic sublattice were evident viz. Γ4(Gx, Ay, Fz) → Γ1(Ax, Gy, Cz) → Γ2(Fx, Cy, Gz) at temperatures of 49 and 26 K. As magnetic field along c axis increases, the sample resumes Γ4 state in place of Γ1 state. Along c axis, field- induced transition from Γ1 to Γ4 is feasible. Studies on hybrid organic-inorganic perovskite compounds have also been carried out on heterometallic [(CH3)2NH2]Mn0.5Ni0.5(HCOO)3 and [(CH3)2 NH2]Co0.5Ni0.5(HCOO)3 which were found to crystallize in trigonal space group R-3c at room temperature and order antiferromagnetically with weak ferromagnetism induced by spin canting at 17 and 8 K, respectively. Hydrogen bond ordering leads to spontaneous polarization and structural transition occurs from R-3c to Cc through mixed phase. This is reflected in impedance data also. Highlights of major findings in different chapters and a general conclusion to this study are presented at the end.