Articles you may be interested inConnectivity and critical current density of in-situ processed MgB2 superconductors: Effect of excess Mg and non-carbon based additives A new scaling relation for n-AlN doped superconducting MgB2SiC and carbon nanotube distinctive effects on the superconducting properties of bulk Mg B 2Series of ex-situ polycrystalline MgB 2 bulk samples, by adding different additives like more of excess Mg (5 wt. %), nanoparticles of Ag (3 wt. %), and SiC (10 wt. %) to a previously optimized composition MgB 2 þ Mg (5 wt. %), were prepared by solid state synthesis route. Detailed investigations were carried out by XRD, SEM, and thermoelectric power S(T), resistivity q(T), and magnetization M(B) at temperatures T ¼ 4.2-300 K and applied fields B ¼ 0-8 T. All the samples typically show low connectivity (i.e., normal state current carrying cross section $0.9%-3%). The effect of different additives was different on the critical current density (J c ) of the samples. The J c , for instance at T ¼ 4.2 K and B ¼ 1 T, varied between 4.8 Â 10 7 and 2.8 Â 10 8 A/m 2 for various samples. In comparison to the previously optimized values, the J c was enhanced by further addition of 5 wt. % Mg and degraded both by nano-SiC and nano-Ag addition. However, many of the other properties of the samples were not much affected. For instance, the samples did not show any change in the superconducting onsets, S(T) and the parallel upper critical field (B jj c2 (T) $ 11-13 T at 20 K and 20-21 T at 4.2 K). The J c (B) dependence also shows similar behavior in all the samples, where the J c is found to scale as B À1 up to a sample independent crossover field B cr $ 2 T and 1.3 T at T ¼ 4.2 and 20 K, respectively. At higher fields B > B cr , the J c (B) curves branch out and decrease rapidly towards zero at a sample dependent characteristic field. We try to understand these results quantitatively in terms of changes in connectivity, pinning, and anisotropy driven percolation. However, all our results and analysis point out that the intra-particle regions stay unaffected and mainly the inter-particle regions get affected by the additives leading to the J c variation in the weakly connected samples.