Vortex dynamics as a function of field orientation in BaFe1.9Ni0.1As2

Vortex dynamics in a multiband anisotropic superconductor, such as the Fe based superconductors, is interesting and potentially important for applications. In this study we examine flux-creep data for fields along the second magnetization peak observed in M(H) curves of BaFe1.9Ni0.1As2 for H ‖ c-axis, H ‖ ab-planes and H forming a 45° angle with ab-planes. We find that the M–H loops taken from the different field directions can be collapsed onto a single universal curve at all temperatures with a simple scaling factor equivalent to the superconducting anisotropy, showing that the vortex pinning is not only isotropic and three-dimensional but most likely related to point-like defects. The resulting critical currents, however, taken from the Bean model appear to show enhanced low field pinning for H ‖ c. The features in the vortex dynamics also differ in different field orientations and show no direct correlation with the second magnetization peak Hp as is the case with a direct crossover in pinning regimes. Isofield plots of the scaled activation energy obtained from flux-creep data are found to be a smooth function of temperature as the Hp(T) line is crossed, consistent with a single type of pinning regime operating at this field, independent of field orientation. The functional form of the Hp(T) lines in the resulting phase diagrams also support this view.

[1]  H. Wen Overview on the physics and materials of the new superconductor KxFe2−ySe2 , 2012, Reports on progress in physics. Physical Society.

[2]  S. Hayden,et al.  Polarized neutron scattering studies of magnetic excitations in electron-overdoped superconducting BaFe1.85Ni0.15As2 , 2012, 1205.3730.

[3]  R. Prozorov,et al.  Anisotropy of strong pinning in multi-band superconductors , 2012, 1205.1741.

[4]  C. Senatore,et al.  Temperature and time scaling of the peak-effect vortex configuration in FeTe 0.7 Se 0.3 , 2012, 1204.5934.

[5]  C. S. Sundar,et al.  Critical current density and magnetic phase diagrams of BaFe1.29Ru0.71As2 single crystals , 2012, 1204.0339.

[6]  Huiqian Luo,et al.  Fishtail and vortex dynamics in the Ni-doped iron pnictide BaFe1.82Ni0.18As2 , 2011, 1106.2248.

[7]  B. Buchner,et al.  Fishtail effect and vortex dynamics in LiFeAs single crystals , 2010, 1009.4896.

[8]  P. Mandal,et al.  The magnetization of PrFeAsO0.60F0.12 superconductor , 2010, 1002.0208.

[9]  Jr.,et al.  Flux dynamics associated with the second magnetization peak in the iron pnictide Ba 1 − x K x Fe 2 As 2 , 2010, 1008.2880.

[10]  T. Xiang,et al.  Anisotropic neutron spin resonance in superconducting BaFe(1.9)Ni(0.1)As(2) , 2010, 1003.1926.

[11]  R. Kopeliansky,et al.  Possibility of vortex lattice structural phase transition in the superconducting pnictide Ba ( Fe 0.925 Co 0.075 ) 2 As 2 , 2010 .

[12]  C. Trautmann,et al.  The effect of columnar defects on the pinning properties of NdFeAsO0.85 conglomerate particles , 2009, 0907.0217.

[13]  Karen Willcox,et al.  Kinetics and kinematics for translational motions in microgravity during parabolic flight. , 2009, Aviation, space, and environmental medicine.

[14]  Yi Yin,et al.  Scanning tunneling spectroscopy and vortex imaging in the iron pnictide superconductor BaFe1.8Co0.2As2. , 2008, Physical review letters.

[15]  M. Norman High-temperature superconductivity in the iron pnictides , 2008 .

[16]  X. Dai,et al.  Observation of Fermi-surface–dependent nodeless superconducting gaps in Ba0.6K0.4Fe2As2 , 2008, 0807.0419.

[17]  H. Wen,et al.  Magnetization relaxation and collective vortex pinning in the Fe-based superconductor SmFeAsO(0.9)F(0.1) , 2008, 0806.0980.

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

[19]  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.

[20]  Y. M. Cho,et al.  Topological objects in two-gap superconductor , 2006, cond-mat/0601347.

[21]  A. Shaulov,et al.  Peak effect and square-to-rhombic vortex lattice transition in La2-xSrxCuO4 , 2005 .

[22]  E. Babaev,et al.  Semi-Meissner state and neither type-I nor type-II superconductivity in multicomponent systems , 2004, cond-mat/0411681.

[23]  E. Babaev Vortices with fractional flux in two-gap superconductors and in extended faddeev model. , 2001, Physical review letters.

[24]  G. I. Menon Phase behavior of type-II superconductors with quenched point pinning disorder: A phenomenological proposal , 2001, cond-mat/0103013.

[25]  Niels Grønbech-Jensen,et al.  Disordering transitions in vortex matter: peak effect and phase diagram , 2000, cond-mat/0008350.

[26]  Niels Grønbech-Jensen,et al.  Static and dynamic coupling transitions of vortex lattices in disordered anisotropic superconductors. , 2000, Physical review letters.

[27]  R. Prozorov,et al.  Plastic Vortex Creep in YBa{sub {bold 2}}Cu{sub {bold 3}}O{sub {bold 7{minus}}}{ital x} Crystals , 1996 .

[28]  A. Malozemoff,et al.  Magnetic relaxation in high-temperature superconductors , 1996 .

[29]  Vinokur,et al.  Plastic Vortex Creep in YBa2Cu3O7-x Crystals. , 1996, Physical review letters.

[30]  Coulter,et al.  Dependence of the flux-creep activation energy on the magnetization current for a La1.86Sr0.14CuO4 single crystal. , 1991, Physical review. B, Condensed matter.

[31]  W. Webb,et al.  FLUX CREEP IN TYPE-II SUPERCONDUCTORS. , 1969 .

[32]  C. P. Bean,et al.  Magnetization of High-Field Superconductors , 1964 .