journal article·2022-11

Observation of structural change-driven Griffiths to non-Griffiths-like phase transformation in Pr2-xSrxCoFeO6 (x = 0 to 1)

Arkadeb Pal, Khyati Anand, Dheeraj Kumar, Amish G. Joshi, Peter Tsung-Wen Yen, Shin-Ming Huang, H.D. Yang, A.K. Ghosh, Sandip Chatterjee

Publisher page

Abstract

The study of crystal structure, electronic structure, transport, and magnetic properties of heterovalent Sr 2+ doped Pr 2-xSr xCoFeO 6 (x = 0.0 to 1.0) system have been done. Crystal structure study reveals an occurrence of structural change from orthorhombic ( Pnma) to tetragonal ( I4/m) phase above x = 0.6. A sudden transformation of the Griffiths-like to non-Griffiths-like magnetic phase is observed as the system changes its crystal structure from Pnma to I4/m. The X-ray photoemission spectroscopy (XPS) study suggests for the existence of mixed oxidation states of the B-site ions viz., Co 3+/Co 4+ and Fe 3+/Fe 4+, and it also indicates an increase in the mean oxidation states owing to the hole substitution (Sr 2+). The temperature variation of the electrical resistivity of the studied systems follows two different transport mechanisms, such as the variable range hopping (VRH) (in the lower temperature region) and small polaron hoping (SPH) (in the higher temperature region) models. Dc magnetization study shows that a local competing ferromagnetic (FM) exchange interaction increases with Sr doping. Finally, the ac susceptibility study reveals breaking of the long-range-ordering in the system x = 1.0, which appears to be related to the structural change and enhanced spin frustration due to increased competing local FM exchange interactions. In addition, electronic density of states (DOS) calculations of PrSrCoFeO 6 (i.e. x = 1.0) using the density functional theory (DFT) have been performed for various Co/Fe atomic distributions. For most of the Co/Fe atomic distributions studied, the calculations show that the total energy of the system with FM coupling among spins has slightly lower energy than that for antiferromagnetic (AFM) coupling.
Source: expertdata · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Magnetic and transport properties of perovskites and related materials · Advanced Condensed Matter Physics · Multiferroics and related materials

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (50)

Show source-provided references
1. Epitaxial BiFeO 3 multiferroic thin film heterostructures10.1126/science.1080615 ↗
2. Multiferroics: a magnetic twist for ferroelectricity10.1038/nmat1804 ↗
3. Observation of coupled magnetic and electric domains10.1038/nature01077 ↗
4. Large magnetic-entropy change above 300 K in CMR materials10.1016/S0304-8853(02)01151-4 ↗
5. Magnetocapacitance and magnetoresistance near room temperature in a ferromagnetic semiconductor: La2NiMnO610.1002/adma.200500737 ↗
6. Near-room-temperature colossal magnetodielectricity and multiglass properties in partially disordered La2NiMnO610.1103/PhysRevLett.108.127201 ↗
7. Room-temperature magnetoresistance in an oxide material with an ordered double-perovskite structure10.1038/27167 ↗
8. Long-range Ni/Mn structural order in epitaxial double perovskite La2NiMnO6 thin films10.1103/PhysRevB.79.224421 ↗
9. Multiferroic behavior in the double-perovskite Lu2MnCoO610.1103/PhysRevB.84.134427 ↗
10. Griffiths phase-like behavior and spin-phonon coupling in double perovskite Tb2NiMnO610.1063/1.3671674 ↗
11. Disordered ferromagnetism in Ho2NiMnO6 double perovskite10.1088/0953-8984/29/2/025804 ↗
12. The evolution of multiferroics10.1038/natrevmats.2016.46 ↗
13. Raman spectroscopy of ordered double perovskite La2CoMnO6 thin films10.1103/PhysRevB.75.104118 ↗
14. Magnetoelectric and structural properties of Y2CoMn O6: The role of antisite defects10.1103/PhysRevB.93.214401 ↗
15. Investigation of multi-mode spin–phonon coupling and local B-site disorder in Pr2CoFeO6 by Raman spectroscopy and correlation with its electronic structure by XPS and XAS studies10.1088/1361-648X/ab144f ↗
16. Probing the Griffiths like phase, unconventional dual glassy states, giant exchange bias effects and its correlation with its electronic structure in Pr2−xSrxCoMnO610.1088/1361-648X/ab5326 ↗
17. Antisite disorder driven spontaneous exchange bias effect in La2-xSrxCoMnO6 (0 ≤ x ≤ 1)10.1088/0953-8984/28/8/086003 ↗
18. Giant zero field cooled spontaneous exchange bias effect in phase separated La1.5Sr0.5CoMnO610.1063/1.4855135 ↗
19. Colossal Magnetoresistance in Manganites as a Multicritical Phenomenon10.1103/PhysRevLett.90.197201 ↗
20. Colossal magnetoresistant materials: the key role of phase separation10.1016/S0370-1573(00)00121-6 ↗
21. Colossal magnetoresistance is a Griffiths singularity10.1103/PhysRevLett.88.197203 ↗
22. Nonanalytic Behavior Above the Critical Point in a Random Ising Ferromagnet10.1103/PhysRevLett.23.17 ↗
23. On the eigenvalue spectrum of the susceptibility matrix for random spin systems10.1088/0022-3719/15/23/008 ↗
24. Short-range ferromagnetic correlations in the spin-chain compound Ca3CoMnO610.1103/PhysRevB.84.054435 ↗
25. A Griffiths-like phase in antiferromagnetic R0.5Eu0.5MnO3 (R = Pr, Nd, Sm)10.1088/0953-8984/25/6/066006 ↗
26. Identification of a Griffiths singularity in a geometrically frustrated antiferromagnet10.1103/PhysRevB.95.054401 ↗
27. B-site disorder driven multiple-magnetic phases: Griffiths phase, re-entrant cluster glass, and exchange bias in Pr2CoFeO610.1063/1.5094905 ↗
28. Griffiths phase behaviour in a frustrated antiferromagnetic intermetallic compound10.1038/srep15801 ↗
29. Signature of a Griffiths phase in layered canted antiferromagnet Sr2IrO410.1016/j.jmmm.2018.07.091 ↗
30. Non-Griffiths-like clustered phase above the Curie temperature of the doped perovskite cobaltite La1−xSrxCoO310.1103/PhysRevB.76.014401 ↗
31. Correlation between phase competition and the nucleation of a Griffiths-like phase in (La1-yPry)0.7Ca0.3Mn16/18O310.1209/0295-5075/84/47009 ↗
32. Evolution from Griffiths like phase to non-Griffiths like phase with Y doping in (La1-xYx)0.7Ca0.3MnO310.1016/j.jmmm.2018.08.028 ↗
33. Spin reorientation and disordered rare earth magnetism in Ho2FeCoO610.1088/1361-648X/aa919e ↗
34. Observation of spin glass state in weakly ferromagnetic Sr2FeCoO6 double perovskite10.1063/1.3686137 ↗
35. Irreversible metamagnetic transition and magnetic memory in small-bandwidth manganite Pr1-xCaxMnO3(x=0.00.5)10.1088/0953-8984/24/21/216002 ↗
36. Praseodymium 3 d - and 4 d -core photoemission spectra of Pr2O310.1103/PhysRevB.44.5465 ↗
37. Enhancement of thermoelectric power factor by inducing octahedral ordering in La2−xSrxCoFeO610.1103/PhysRevB.99.174105 ↗
38. X-ray photoemission measurements of La1-xCaxCoO310.1103/PhysRevB.54.14938 ↗
39. Electronic structure and magnetic states in La1−xSrxCoO310.1103/PhysRevB.56.1290 ↗
40. Synthesis and investigation of structural and electronic properties of Pr1-xCaxFeO3 (0≤x≤0.2) compounds10.1016/j.physb.2005.04.036 ↗
41. Magnetic and transport properties driven by Sr substitution in polycrystalline Pr1-xSrxCoO3 (0.1 ≤ x ≤ 0.5) cobaltites10.1063/1.5039617 ↗
42. Relaxor-like dielectric behavior in La2NiMnO6 double perovskite ceramics10.1016/j.ssc.2009.02.028 ↗
43. Multifunctional behaviour in B-site disordered double perovskite EuPrCoMnO610.1088/1361-6463/ac5fd4 ↗
44. Disorder effect on the electronic and magnetic properties of Sr2FeCoO6: A density-functional theoretical investigation10.1063/1.3653238 ↗
45. Large magnetoresistance and Jahn-Teller effect in Sr2FeCoO610.1140/epjb/e2012-30264-2 ↗
46. Strain-driven spin-state transition and superexchange interaction in LaCoO3 initio study10.1103/PhysRevB.86.014430 ↗
47. Theory of the Role of Covalence in the Perovskite-Type Manganites [La, M(II)]MnO310.1103/PhysRev.100.564 ↗
48. Structural correlation with the Griffiths phase in disordered magnetic systems10.1103/PhysRevB.98.184419 ↗
49. Evolution of Curie-Weiss behavior and cluster formation temperatures in Ru-doped Sm0.55Sr0.45MnO310.1103/PhysRevB.82.172401 ↗
50. Nature of short-range ferromagnetic ordered state above Tc in double perovskite La2NiMnO610.1063/1.3459141 ↗