Anisotropy and penetration depth of MgB2 from 11B NMR

The 11B NMR spectra in polycrystalline MgB2 were measured for several magnetic fields (1.97 and 3.15 T) as a function of temperature from 5 to 40 K. The composite spectra in the superconducting state can be understood in terms of anisotropy of the upper critical field, γH, which is determined to be 5.4 at low temperature. Using Brandt's algorithm (Brandt 1997 Phys. Rev. Lett. 78 2208) the full spectrum, including satellites, was simulated for the temperature 8 K and a magnetic field of 1.97 T. The penetration depth λ was determined to be 1152 ± 50 Å, and the anisotropy of the penetration depth, γλ, was estimated to be close to one at low temperature. Therefore, our findings establish that there are two different anisotropies for upper critical field and penetration depth at low temperatures.

[1]  Sung-Ik Lee,et al.  Measurement of the anisotropy ratios in MgB2 single crystals , 2006 .

[2]  C. Dewhurst,et al.  Measuring the penetration depth anisotropy in Mg B 2 using small-angle neutron scattering , 2005, cond-mat/0511376.

[3]  J. Karpinski,et al.  Temperature-dependent anisotropy of the penetration depth and coherence length of MgB2. , 2005, Physical review letters.

[4]  A. Wisniewski,et al.  Anisotropy in superconducting MgB2: a comparison of SQUID and torque measurements , 2004 .

[5]  R. Ribeiro,et al.  Anisotropy and internal-field distribution of MgB2 in the mixed state at low temperatures , 2004, cond-mat/0405495.

[6]  K. H. Kang,et al.  Penetration depth and Hc2 anisotropy of MgB2 by 11B NMR , 2004 .

[7]  M. Fardis,et al.  11B NMR Study of Pure and Lightly Carbon-Doped MgB2 Superconductors , 2004, cond-mat/0402668.

[8]  K. H. Kim,et al.  Anisotropies of the lower and upper critical fields in MgB2 single crystals. , 2004, Physical review letters.

[9]  O. Fischer,et al.  Vortex imaging in magnesium diboride with H ⊥ c , 2003 .

[10]  W. Kwok,et al.  Two-band effects in the angular dependence of Hc2 of MgB2 single crystals , 2003, cond-mat/0308319.

[11]  C. Dewhurst,et al.  Effects of two-band superconductivity on the flux-line lattice in magnesium diboride. , 2003, Physical review letters.

[12]  M. Maple,et al.  Vortex- and Bragg-glass phases in bulk MgB2 , 2003 .

[13]  V. Kogan,et al.  Anisotropy parameters of superconducting MgB2 , 2002, cond-mat/0212383.

[14]  S. Louie,et al.  The origin of the anomalous superconducting properties of MgB2 , 2002, Nature.

[15]  J. Kortus,et al.  Multiband model for penetration depth in MgB2 , 2002, cond-mat/0205154.

[16]  V. Kogan Macroscopic anisotropy in superconductors with anisotropic gaps , 2002, cond-mat/0204038.

[17]  P. Canfield,et al.  Temperature-dependent Hc2 anisotropy in MgB2 as inferred from measurements on polycrystals , 2002, cond-mat/0201085.

[18]  A. Wisniewski,et al.  Temperature and field dependence of the anisotropy of MgB2. , 2001, Physical review letters.

[19]  E. Sigmund,et al.  Spatially resolved electronic structure inside and outside the vortex cores of a high-temperature superconductor , 2001, Nature.

[20]  M. Fardis,et al.  $^{11}$B NMR detection of the magnetic field distribution in the mixed superconducting state of MgB$_2$ , 2001, cond-mat/0107511.

[21]  J. Nagamatsu,et al.  Superconductivity at 39 K in magnesium diboride , 2001, Nature.

[22]  P. Canfield,et al.  Thermodynamic and transport properties of superconducting Mg10B2. , 2001, Physical review letters.

[23]  E. Brandt,et al.  Solution of the anisotropic Ginzburg-Landau theory by the iterative method , 2000 .

[24]  R. Kiefl,et al.  μSR studies of the vortex state in type-II superconductors , 2000 .

[25]  E. Brandt Precision Ginzburg-Landau Solution of Ideal Vortex Lattices for Any Induction and Symmetry , 1997 .

[26]  L. Drain The Broadening of Magnetic Resonance Lines due to Field Inhomogeneities in Powdered Samples , 1962 .

[27]  P. Canfield,et al.  Penetration depth anisotropy in MgB2 single crystals and powders , 2006 .

[28]  M. Fardis,et al.  Magnetization and 11B NMR study of Mg1-xAlxB2 superconductors , 2002 .