Neutron powder diffraction study on the non-superconducting phases of ThFeAsNO () iron pnictide
arXiv:1907.06531 · doi:10.1088/0256-307X/36/10/107403
Abstract
We use neutron powder diffraction to study on the non-superconducting phases of ThFeAsNO with . In our previous results on the superconducting phase ThFeAsN with 30 K, no magnetic transition is observed by cooling down to 6 K, and possible oxygen occupancy at the nitrogen site is shown in the refinement(H. C. Mao \emph{et al.}, EPL, 117, 57005 (2017)). Here, in the oxygen doped system ThFeAsNO, two superconducting region ( and ) have been identified by transport experiments (B. Z. Li \emph{et al.}, J. Phys.: Condens. Matter 30, 255602 (2018)). However, within the resolution of our neutron powder diffraction experiment, neither the intermediate doping nor the heavily overdoped compound shows any magnetic order from 300 K to 4 K. Therefore, while it shares the common phenomenon of two superconducting domes as most of 1111-type iron-based superconductors, the magnetically ordered parent compound may not exist in this nitride family.
arXiv comment4 pages, 4 figures
References in corpus (35)
- Magnetic Order versus superconductivity in the Iron-based layered La(O1-xFx)FeAs systems
- Superconductivity in Iron Compounds
- Magnetic order in BaFe2As2, the parent compound of the FeAs based superconductors in a new structural family
- Antiferromagnetic order and spin dynamics in iron-based superconductors
- First-order magnetic and structural phase transitions in FeSeTe
- High Temperature Superconductivity in Iron Pnictides and Chalcogenides
- The electronic phase diagram of the LaO1-xFxFeAs superconductor
- A Novel Large Moment Antiferromagnetic Order in K0.8Fe1.6Se2 Superconductor
- Exploration of new superconductors and functional materials and fabrication of superconducting tapes and wires of iron pnictides
- Two-dome structure in electron-doped iron arsenide superconductors
- Common Crystalline and Magnetic Structure of superconducting A2Fe4Se5
- Magnetically-Driven Suppression of Nematic Order in an Iron-Based Superconductor
- Superconductivity-induced reentrance of orthorhombic distortion in Ba1-xKxFe2As2
- Bipartite magnetic parent phases in the iron-oxypnictide superconductor
- Hedgehog spin-vortex crystal stabilized in a hole-doped iron-based superconductor
- Superconductivity in LaFeAsPO: effect of chemical pressures and bond covalency
- Spin fluctuations in iron pnictides and chalcogenides: From antiferromagnetism to superconductivity
- A New ZrCuSiAs-Type Superconductor: ThFeAsN
- Magnetic order in CaFe1-xCoxAsF (x = 0, 0.06, 0.12) superconductor compounds
- Antiferromagnetic order and superlattice structure in nonsuperconducting and superconducting RbyFe(1.6+x)Se2
- Detection of antiferromagnetic ordering in heavily doped LaFeAsO1-xHx pnictide superconductors using nuclear-magnetic-resonance techniques
- New Superconductivity Dome in LaFeAsOF Accompanied by Structural Transition
- Superconductivity induced by hydrogen anion substitution in 1111-type iron arsenides
- Emergence of Novel Antiferromagnetic Order Intervening between Two Superconducting Phases in LaFe(As_1-x_P_x_)O: 31P-NMR Studies
- Evolution of the Phase Diagram of LaFePAsOF ( = 0 -- 0.1)
- Antiferromagnetic order in CaK(Fe[1-x]Ni[x])4As4 and its interplay with superconductivity
- Relationship between Superconductivity and Antiferromagnetism in LaFe(AsP)O Revealed by P-NMR
- Multigap superconductivity in ThAsFeN investigated using muSR measurements
- High- superconductivity in undoped ThFeAsN
- ThFeAsN in Relation to Other Iron-Based Superconductors
- Two Fermi surface states and two -rising mechanisms revealed by transport properties in FePAsOF (=La, Pr and Nd)
- Neutron powder diffraction study on the iron-based nitride superconductor ThFeAsN
- Peculiar Phase Diagram with Isolated Superconducting Regions in ThFeAsNO
- Three superconducting phases with different categories of pairing in hole- and electron-doped LaFeAsPO
- Structural Phase Transition, Antiferromagnetism and Two Superconducting Domes in LaFeAsOF (0 0.75)