Magnetic Phase Transitions in NdCoAsO
arXiv:0912.4237 · doi:10.1103/PhysRevB.81.104405
Abstract
Magnetization measurements reveal that NdCoAsO undergoes three magnetic phase transitions below room temperature. The crystal and magnetic structures of NdCoAsO have been determined by powder neutron diffraction, and the effects of the phase transitions on physical properties are reported. Near 69 K a ferromagnetic state emerges with a small saturation moment of about 0.2 Bohr magnetons, likely on Co atoms. At 14 K the material enters an antiferromagnetic state with propagation vector (0 0 1/2) and small ordered moments (~0.4 Bohr magnetons) on Co and Nd. Near 3.5 K a third transition is observed, and corresponds to the antiferromagnetic ordering, with the same propagation vector, of larger moments on Nd reaching 1.30(2) Bohr magnetons at 1.4 K. In addition, transport properties and heat capacity results are presented, and show anomalies at all three phase transitions.
Some minor changes made, and lower temperature neutron diffraction results are included. Accepted for publication in Physical Review B
References in corpus (15)
- Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2
- Magnetic Order versus superconductivity in the Iron-based layered La(O1-xFx)FeAs systems
- Superconductivity at 22 K in Co-doped BaFe2As2 Crystals
- Spin density wave anomaly at 140 K in the ternary iron arsenide BaFe2As2
- LiFeAs: An Intrinsic FeAs-based Superconductor with Tc = 18K
- Superconductivity in Co-doped LaFeAsO
- Transition of stoichiometricSr2VO3FeAs to a superconducting state at 37.2 K
- Phase transitions in LaFeAsO: structural, magnetic, elastic, and transport properties, heat capacity and Mossbauer spectra
- Contrasting Spin Dynamics Between Underdoped and Overdoped Ba(Fe[1-x]Co[x])2As2
- Electron Correlations in the Low Carrier Density LaFeAsO0.89F0.11 Superconductor (Tc = 28 K)
- Itinerant Ferromagnetism in layered crystals LaCoOX (X = P, As)
- Structure and Magnetic Order in the NdFeAs(O,F) Superconductor System
- Renormalized behavior and proximity to a magnetic quantum critical point in BaCoAs
- Influence of the rare-earth element on the effects of the structural and magnetic phase transitions in CeFeAsO, PrFeAsO, and NdFeAsO
- Superconductivity in NdFe1-xCoxAsO (0.05 < x < 0.20) and rare-earth magnetic ordering in NdCoAsO
Cited by in corpus (23)
- A variable temperature study of the crystal and magnetic structures of the giant magnetoresistant materials LnMnAsO (Ln = La, Nd)
- Two successive field-induced spin-flop transitions in single-crystalline CaCoAs
- Nd induced Mn spin-reorientation transition in NdMnAsO
- Short- and long-range magnetic order in LaMnAsO
- Magnetic phase transitions in SmCoAsO
- Local moments and symmetry breaking in metallic PrMnSbO
- Metamagnetic transition in CaSrCoAs( = 0 and 0.1) single crystals
- Interplay between Co-3d and Ce-4f magnetism in CeCoAsO
- Synthesis, magnetization and magneto transport study of RECoPO (RE = La, Nd & Sm)
- Large Magnetoresistance Effects in CoAsO with a Ferromagnetic-Antiferromagnetic Transition
- Tunable interplay between 3d and 4f electrons in Co-doped iron pnictides
- Intriguing complex magnetism of Co in RECoAsO (RE=La, Nd and Sm)
- Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 to 1.0)
- Magnetic phase diagram in the Co-rich side of LnCo1-xFexAsO (Ln=La, Sm) system
- Competing magnetic phases and field-induced dynamics in DyRuAsO
- Structural and Magnetic Phase Transitions in NdCoAsO under High Pressures
- Anisotropic spin-fluctuations in SmCoPO revealed by 31^P NMR measurement
- Interplay of Sm4f and Co3d spins in SmCoAsO
- Local electromagnetic properties of magnetic pnictides: A comparative study probed by NMR measurement
- Iron substitution in NdCoAsO: crystal structure and magnetic phase diagram
- Common effect of chemical and external pressures on the magnetic properties of CoPO ( = La, Pr, Nd, Sm). II
- Evolution of superconductivity in PrFe1-xCoxAsO with x = 0.0 to 1.0
- Magnetocrystalline anisotropic effect in GdCoFeAsO ()