Narrow superconducting window in LaFe 1 − x Ni x AsO

We have studied Ni-substitution effect in ${\text{LaFe}}_{1\ensuremath{-}x}{\text{Ni}}_{x}\text{AsO}$ $(0\ensuremath{\le}x\ensuremath{\le}0.1)$ by the measurements of x-ray diffraction, electrical resistivity, magnetic susceptibility, and heat capacity. The nickel doping drastically suppresses the resistivity anomaly associated with spin-density-wave ordering in the parent compound. Superconductivity emerges in a narrow region of $0.03\ensuremath{\le}x\ensuremath{\le}0.06$ with the maximum ${T}_{c}$ of 6.5 K at $x=0.04$, where enhanced magnetic susceptibility shows up. The upper critical field at zero temperature is estimated to exceed the Pauli paramagnetic limit. The much lowered ${T}_{c}$ in comparison with ${\text{LaFeAsO}}_{1\ensuremath{-}x}{\text{F}}_{x}$ system is discussed.

[1]  H. Hosono,et al.  Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF , 2008, 0811.1147.

[2]  Q. Tao,et al.  Superconductivity induced by Ni doping in BaFe2As2 single crystals , 2008, 0809.2009.

[3]  E. Abrahams,et al.  Iron pnictides as a new setting for quantum criticality , 2008, Proceedings of the National Academy of Sciences.

[4]  David J. Singh,et al.  Superconductivity at 22 K in Co-doped BaFe2As2 crystals. , 2008, Physical review letters.

[5]  E. A. Payzant,et al.  Phase Transitions in LaFeAsO: Structural, Magnetic, Elastic, and Transport Properties, Heat Capacity and Mössbauer Spectra , 2008, 0806.3878.

[6]  H. Hosono,et al.  Ferromagnetic spin fluctuation in LaFeAsO 1 − x F x , 2008, 0806.3304.

[7]  Gang Li,et al.  Structural and magnetic phase diagram of CeFeAsO(1- x)F(x) and its relation to high-temperature superconductivity. , 2008, Nature materials.

[8]  X. H. Chen,et al.  Anisotropy in the electrical resistivity and susceptibility of superconducting BaFe2As2 single crystals. , 2008, Physical review letters.

[9]  D. Christen,et al.  Two-band superconductivity in LaFeAsO0.89F0.11 at very high magnetic fields , 2008, Nature.

[10]  M. Knupfer,et al.  High-field pauli-limiting behavior and strongly enhanced upper critical magnetic fields near the transition temperature of an arsenic-deficient LaO0.9F0.1FeAs1-delta superconductor. , 2008, Physical review letters.

[11]  Liling Sun,et al.  Superconductivity at 55 K in Iron-Based F-Doped Layered Quaternary Compound Sm[O1-xFx] FeAs , 2008 .

[12]  Guizhen Wu,et al.  Superconductivity at 43 K in SmFeAsO1-xFx , 2008, Nature.

[13]  T. Kamiya,et al.  Nickel-based layered superconductor, LaNiOAs , 2008, 0805.4340.

[14]  Jiansheng Wu,et al.  Theory of the magnetic moment in iron pnictides. , 2008, Physical review letters.

[15]  Z. Tes̆anović,et al.  Multiband magnetism and superconductivity in Fe-based compounds , 2008, 0804.4678.

[16]  Z. Ren,et al.  Thorium-doping–induced superconductivity up to 56 K in Gd1−xThxFeAsO , 2008, 0804.4290.

[17]  S. W. Kim,et al.  Crystallographic phase transition and high-Tc superconductivity in LaFeAsO:F , 2008, 0804.3569.

[18]  E. Abrahams,et al.  Strong correlations and magnetic frustration in the high Tc iron pnictides. , 2008, Physical review letters.

[19]  X. Wen,et al.  Spin-triplet p -wave pairing in a three-orbital model for iron pnictide superconductors , 2008, 0804.1739.

[20]  Chaoxing Liu,et al.  Minimal two-band model of the superconducting iron oxypnictides , 2008, 0804.1113.

[21]  H. Mook,et al.  Magnetic order close to superconductivity in the iron-based layered LaO1-xFxFeAs systems , 2008, Nature.

[22]  D. Christen,et al.  Very High Field Two-Band Superconductivity in LaFeAsO_0.89F_0.11 , 2008, 0804.0485.

[23]  J. Berry,et al.  Diamagnetic Corrections and Pascal's Constants , 2008 .

[24]  Fu-Chun Zhang,et al.  Even parity, orbital singlet, and spin triplet pairing for superconducting LaFeAsO1-xFx. , 2008, Physical review letters.

[25]  Gang Li,et al.  Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeO1-xFxFeAs. , 2008, Physical review letters.

[26]  Gang Li,et al.  Competing orders and spin-density-wave instability in La(O1−xFx)FeAs , 2008, 0803.3426.

[27]  R. Arita,et al.  Unconventional pairing originating from the disconnected Fermi surfaces of superconducting LaFeAsO1-xFx. , 2008, Physical review letters.

[28]  Zhong-Yi Lu,et al.  Iron-based layered compound LaFeAsO is an antiferromagnetic semimetal , 2008, 0803.3286.

[29]  Xiyu Zhu,et al.  Superconductivity at 25 K in hole-doped (La1-xSrx)OFeAs , 2008, 0803.3021.

[30]  M. Johannes,et al.  Unconventional superconductivity with a sign reversal in the order parameter of LaFeAsO1-xFx. , 2008, Physical review letters.

[31]  L. Boeri,et al.  Is LaFeAsO1-xFx an electron-phonon superconductor? , 2008, Physical review letters.

[32]  T. Xiang,et al.  Strong-coupling superconductivity in the nickel-based oxypnictide LaNiAsO 1-x F x , 2008, 0803.2572.

[33]  Yuan Yao,et al.  Doping-dependent phase diagram of LaOMAs (M=V–Cu) and electron-type superconductivity near ferromagnetic instability , 2008, 0803.1282.

[34]  M. Du,et al.  Density functional study of LaFeAsO(1-x)F(x): a low carrier density superconductor near itinerant magnetism. , 2008, Physical review letters.

[35]  Hideo Hosono,et al.  Iron-based layered superconductor La[O(1-x)F(x)]FeAs (x = 0.05-0.12) with T(c) = 26 K. , 2008, Journal of the American Chemical Society.

[36]  Orlando,et al.  3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O. , 1987, Physical review. B, Condensed matter.

[37]  E. Helfand,et al.  Temperature and Purity Dependence of the Superconducting Critical Field, H c 2 . III. Electron Spin and Spin-Orbit Effects , 1966 .

[38]  Clogston Upper limit for the critical field in hard superconductors. [V/sub 2. 95/Ga, NbâSn,VâSi, V/sub 1. 95/ Ga] , 1962 .

[39]  B. Chandrasekhar A NOTE ON THE MAXIMUM CRITICAL FIELD OF HIGH‐FIELD SUPERCONDUCTORS , 1962 .