16 research outputs found
High transport critical current densities in textured Fe-sheathed Sr1-xKxFe2As2+Sn superconducting tapes
We report the realization of grain alignment in Sn-added Sr1-xKxFe2As2
superconducting tapes prepared by ex-situ powder-in-tube method. At 4.2 K, high
transport critical current densities Jc of 2.5x10^4 A/cm^2 (Ic = 180 A) in
self-field and 3.5x10^3 A/cm^2 (Ic = 25.5 A) in 10 T have been measured. These
values are the highest ever reported so far for Fe-based superconducting wires
and tapes. We believe the superior Jc in our tape samples are due to well
textured grains and strengthened intergrain coupling achieved by Sn addition.
Our results demonstrated an encouraging prospect for application of iron based
superconductors.Comment: 14 pages, 4 figure
Transport properties and anisotropy in rare earth doped CaFe2As2 single crystals with Tc above 40 K
In this paper we report the superconductivity above 40 K in the electron
doping single crystal Ca1-xRexFe2As2 (Re = La, Ce, Pr). The x-ray diffraction
patterns indicate high crystalline quality and c-axis orientation. the
resistivity anomaly in the parent compound CaFe2As2 is completely suppressed by
partial replacement of Ca by rare earth and a superconducting transition
reaches as high as 43 K, which is higher than the value in electron doping
FeAs-122 compounds by substituting Fe ions with transition metal, even
surpasses the highest values observed in hole doping systems with a transition
temperature up to 38 K. The upper critical field has been determined with the
magnetic field along ab-plane and c-axis, yielding the anisotropy of 2~3.
Hall-effect measurements indicate that the conduction in this material is
dominated by electron like charge carriers. Our results explicitly demonstrate
the feasibility of inducing superconductivity in Ca122 compounds via electron
doping using aliovalent rare earth substitution into the alkaline earth site,
which should add more ingredients to the underlying physics of the iron-based
superconductors.Comment: 21 pages, 7 figure
Effect of starting materials on the superconducting properties of SmFeAsO1-xFx tapes
SmFeAsO1-xFx tapes were prepared using three kinds of starting materials. It
shows that the starting materials have an obvious effect on the impurity phases
in final superconducting tapes. Compared with the other samples, the samples
fabricated by SmAs, FeO, Fe2As, and SmF3 have the smallest arsenide impurity
phase and voids. As a result, these samples possess much denser structure and
better grain connectivity. Moreover, among the three kinds of samples
fabricated in this work, this kind of sample has the highest zero-resistivity
temperature ~40 K and largest critical current density ~4600 A/cm^2 in
self-field at 4.2 K. This is the highest Jc values reported so far for
SmFeAsO1-xFx wires and tapes.Comment: 15 pages, 4 figure
Improved transport critical currents in Ag and Pb co-doped BaxK1-xFe2As2 superconducting tapes
Fe-clad BaxK1-xFe2As2 superconducting tapes were fabricated by the ex situ
powder-in-tube method combined with a short high-temperature annealing
technique. The effect of annealing time and different dopants on the transport
properties of the BaxK1-xFe2As2 tapes were systematically studied. By co-doping
with Ag and Pb, the transport critical current density Jc of BaxK1-xFe2As2
tapes was significantly improved in whole field region and the highest
transport Jc was up to 1.4x10^4 A/cm^2 (Ic=100 A) at 4.2K in self field. It is
proposed that the superior Jc in the co-doped samples are due to the combine
effect of Pb doping at low fields and Ag doping at high fields.Comment: 22 pages, 7 figures, to be published in Supercond. Sci. Techno
Morphology and Crystallography of Ausferrite in Austempered Ductile Iron
The microstructure of austempered ductile iron was investigated by electron backscatter diffraction technique. The results show that the orientation relationship between acicular bainitic ferrite and austenite is Greninger–Troiano relationship. A single austenite grain is divided into four packets and each packet contains six variants that share a {011}α (i.e., {111}γ) plane. When two γ grains are twinned, the twins share a {111}γ plane and have seven packets. The adjacent acicular bainitic ferrite plates (or laths) sharing a 〈 001 〉 γ axis have small misorientation of about 5.7°. The adjacent acicular bainitic ferrite plates (or laths) not sharing a 〈 001 〉 γ axis have two high misorientation angles of ~54.3° and ~60.0°. Further, the low angle boundary to high angle boundary ratio is far less than the ratio of the variant pairs with small misorientation to the ones with large misorientation. This work is available for structures obtained as a consequence of the heat treatment of austempering
Superconductivity and phase diagram in Ru-doped SrFe
Single crystals of SrFe2−xRuxAs2 have been successfully synthesized using the FeAs self-flux method. The X-ray diffraction patterns indicate that the substitution of Fe by Ru leads to a decrease of the c parameter. Upon Ru substitution, the resistivity anomaly in the parent compound is progressively suppressed and superconductivity is stabilized at low temperatures for x≥0.45. The superconducting region is dome-like, with an optimal Tc ∼15.5 K found around x=0.667. A phase diagram of temperature vs. doping, based on electrical transport, has been constructed. Results of upper and lower critical field are presented. Our results confirm that the substitution of Fe ions with isoelectronic Ru could suppress the magnetic/structural phase transition in the parent compound, and suggest that there is strong competition between magnetism, structure, and superconductivity in iron-based superconductors
Superconductivity and magnetic properties in SmFe
In this paper the effects of replacing Fe with Co in SmFe1-xCoxAsO (x=0 to 1) are reported. X-ray diffraction patterns indicate that all the samples have formed the ZrCuSiAs-type structure with a space group P4/nmm and a full solid solution forms between SmFeAsO and SmCoAsO. It is found that the antiferromagnetic spin-density-wave (SDW) order in the parent compounds is rapidly suppressed by Co-doping, and superconductivity emerges as 0.05 ≤ x ≤ 0.175. A phase diagram is derived based on the resistivity measurements and a dome-like Tc-vs.-x curve is established. Furthermore, it was shown that the metallic character increases with the addition of more Co. Meanwhile we found that the two magnetic phase transitions in SmCoAsO are suppressed as Co is replaced by Fe. Our work demonstrates that the solid solution has been established in the SmFeAsO-SmCoAsO system. The systemic study in the SmFe1-xCoxAsO system would add more ingredients to the underlying physics of this material
Superconductivity at 22 K in Ir-doped CaFe
In this paper we report superconductivity in single crystals of the new iron-pnictide system CaFe2−xIrxAs2 (x=0, 0.05, 0.10, 0.13) grown by a self-flux solution method and characterized via X-ray, transport and magnetic measurements. The magnetic ordering associated with a structural transition at 160 K present in CaFe2As2 is completely suppressed by substitution of Fe with Ir and superconductivity is induced at a critical temperature Tc=22 K in the sample with x=0.13. We also determined the upper critical fields along the ab-plane and
c-axis. The anisotropy of the CaFe2−xIrxAs2 superconductors determined by the ratio of Habc2 and Hcc2 is estimated to be 1.5–2.2. Our results suggest that superconductivity can also be easily induced in the CaFe2As2 family by substituting the Fe with Ir, at almost the similar maximum transition temperatures as for Co, Ni and Rh doping