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Related papers: Narrow superconducting window in Ni-doped LaFeAsO

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We report the synthesis and characterization of a new electron-doped La-oxypnictide superconductor by partial substitution of lanthanum by thorium. The superconducting transition temperature at about 30.3 K was observed in La0.8Th0.2OFeAs…

Superconductivity · Physics 2009-11-13 J. Prakash , S. J. Singh , S. Patnaik , A. K. Ganguli

Here we report the superconductivity in the LaFeAsO1-xFx system prepared by high pressure synthesis. The highest onset superconducting transition temperature (Tc) in this La-based system is 41.0 K with the nominal composition of…

The phase diagram of NdFe1-xCoxAsO for low cobalt substitution consists of a superconducting dome (0.05 < x < 0.20) with a maximum critical temperature of 16.5(2) K for x = 0.12. The x = 1 end member, NdCoAsO, is an itinerant ferromagnet…

We report the results from resistivity and magnetic measurements on polycrystalline Ce oxypnictide (CeFeAsO1-xFx) samples where x spans from 0.13 to 0.25. We find that the orbital limiting field is as high as 150 T and it systematically…

Superconductivity · Physics 2014-10-27 S. V. Chong , G. V. M. Williams , S. Sambale , K. Kadowaki

We have successfully synthesized one member of LnFeAsO (Ln stands for lanthanides) with Ln=Tb. By partial substitution of Tb$^{3+}$ by Th$^{4+}$, superconductivity with onset $T_{c}$ up to 52 K was observed. In the undoped parent compound,…

Superconductivity · Physics 2008-10-11 Lin-jun Li , Yu-ke Li , Zhi Ren , Yong-kang Luo , Xiao Lin , Mi He , Qian Tao , Zeng-wei Zhu , Guang-han Cao , Zhu-an Xu

The effect of electron doping by trivalent charge state rare-earth ion (RE = La, Ce, Pr, and Nd) substitutions on the superconductivity in BaFe2As2 was examined using epitaxial films. Each of the RE substitutions suppressed the resistivity…

Superconductivity · Physics 2013-07-10 Takayoshi Katase , Hidenori Hiramatsu , Toshio Kamiya , Hideo Hosono

Iron arsenide superconductors based on the material LaFeAsO1-xFx are characterized by a two-dimensional Fermi surface (FS) consisting of hole and electron pockets yielding structural and antiferromagnetic transitions at x = 0. Electron…

A series of (Li$_{0.8}$Fe$_{0.2}$)OHFeSe$_{1-x}$S$_x$ (0 $\leq$ x $\leq$ 1) samples were successfully synthesized via hydrothermal reaction method and the phase diagram is established. Magnetic susceptibility suggests that an…

Superconductivity · Physics 2015-01-07 X. F. Lu , N. Z. Wang , X. G. Luo , G. H. Zhang , X. L. Gong , F. Q. Huang , X. H. Chen

We have investigated experimentally how properties of NdFeAsO0.8F0.2 superconductor affected due to the substitution of the Ca2+/Nd3+ doping. Based on the XRD data refinement, various structural parameters such as lattice parameters, bond…

Superconductivity · Physics 2019-05-29 F. Shahbaz Tehrani , V. Daadmehr

The crystal structure and numerous normal and superconducting state properties of layered tetragonal (P4/nmm) LaFeAsO, with F-doping of 11 %, are reported. Resistivity measurements give an onset transition temperature Tc = 28.2 K, and low…

Superconductivity · Physics 2009-11-13 Athena S. Sefat , Michael A. McGuire , Brian C. Sales , Rongying Jin , Jane Y. Howe , David Mandrus

We report the synthesizing and characterization of the hole doped Ni-based superconductor ($La_{1-x}Sr_{x})ONiAs$. By substituting La with Sr, the superconducting transition temperature $T_c$ is increased from 2.75 K of the parent phase…

Superconductivity · Physics 2013-05-29 Lei Fang , Huan Yang , Peng Cheng , Xiyu Zhu , Gang Mu , Hai-Hu Wen

High-resolution neutron inelastic scattering experiments in applied magnetic fields have been performed on La$_{1.895}$Sr$_{0.105}$CuO$_{4}$ (LSCO). In zero field, the temperature dependence of the low-energy peak intensity at the…

The electrical resistivity (Rxx) and Hall resistivity (Rxy) of LaFeAsO1-xFx have been measured over a wide fluorine doping range 0 =< x =< 0.14 using 60 T pulsed magnets. While the superconducting phase diagram (Tc, x) displays the classic…

Superconductivity · Physics 2015-05-13 Y. Kohama , Y. Kamihara , S. A. Baily , L. Civale , S. C. Riggs , F. F. Balakirev , T. Atake , M. Jaime , M. Hirano , H. Hosono

A series of layered nickel-based LaO$_{1-x}$F$_x$NiAs compounds with x=0 to 0.15 are synthesized by solid state reactions. The pure LaONiAs exhibits bulk superconductivity with Tc $\sim$ 2.75 K. Partial substitution of oxygen by fluorine…

Superconductivity · Physics 2008-08-19 Z. Li , G. F. Chen , J. Dong , G. Li , W. Z. Hu , D. Wu , S. K. Su , P. Zheng , T. Xiang , N. L. Wang , J. L. Luo

The effect of off-plane impurity on superconductivity and non-Fermi-liquid (NFL) behavior in the layered heavy-fermion compound CeCo$_{1-x}$Ni$_x$In$_5$ is investigated by specific heat, magnetization, and electrical resistivity…

A suppression of superconductivity in the late rare earth RFeAsO1-xFx materials is reported. The maximum critical temperature (Tc) decreases from 51 K for R = Tb to 36 K for HoFeAsO0.9F0.1, which has been synthesised under 10 GPa pressure.…

High-quality superconducting LaFeAsO$_{1-x}$F$_{x}$ thin films were grown on single crystalline LaAlO$_{3}$ substrates with critical temperatures (onset) up to 28 K. Resistive measurements in high magnetic fields up to 40 T reveal a…

We argue that the newly discovered superconductivity in a nearly magnetic, Fe-based layered compound is unconventional and mediated by antiferromagnetic spin fluctuations, though different from the usual superexchange and specific to this…

Superconductivity · Physics 2015-05-13 I. I. Mazin , D. J. Singh , M. D. Johannes , M. H. Du

We have employed a new route to synthesize single phase F-doped LaOFeAs compound and confirmed the superconductivity above 20 K in this Fe-based system. We show that the new superconductor has a rather high upper critical field of about 54…

Superconductivity · Physics 2009-11-13 G. F. Chen , Z. Li , G. Li , J. Zhou , D. Wu , J. Dong , W. Z. Hu , P. Zheng , Z. J. Chen , H. Q. Yuan , J. Singleton , J. L. Luo , N. L. Wang

We present a study of the structural and physical properties of directly hole doped LaFe1-xMnxAsO (x = 0.0-0.2) and the influence of charge compensation / electron-doping by additional F doping in LaFe0.9Mn0.1AsO1-yFy (y = 0.1-0.5). High…

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