Preparation, Microstructure, and High-Field Superconducting Properties of Nb3 Sn Doped with Group-III, -IV, -V, and -VI Elements

Abstract
The influence of incorporating elements from groups III, IV, V, and VI into vapor‐deposited Nb3Sn superconducting ribbon on the critical current density in magnetic fields up to 190 kOe has been examined, and the mechanism of the enhancement of Jc by carbon‐containing gases has been investigated. It had been found previously that CO2, CO, and N2, but not O2 or CH4 are effective in increasing Jc. We have now established that the less stable C2H6 and C3H8 are as effective as CO2, and that BCl3 increases Jc to a lesser extent. However, H2S, NH3, and NO decrease Jc compared with an undoped Nb3Sn sample. By optimizing the CO2 concentration in the gas phase, the Jc increase can be as much as a factor of 5; this optimum concentration corresponds to about 2000 ppm carbon in the Nb3Sn vapor‐grown layer, as determined by radioactive tracer and mass spectrographic analyses. Since the solid solubility limit of carbon in Nb3Sn is less than 200 ppm, carbon or carbide in excess of this amount is distributed as a second phase probably along subgrain or grain boundaries where it can effectively pin flux lines, and thereby increase Jc. From extrapolations of Jc1/2vs H , the upper critical fields at 4.2 °K for undoped and BCl3‐ and C2H6‐doped Nb3Sn on stainless‐steel substrates are 184, 194, and 196 kOe, respectively, while for CO2‐doped Nb3Sn on a Nb substrate it is 225 kOe. α = JcH values ranging from 22 to 32×106 kOeA/cm2 were attained for C3H8‐, C2H6‐, and CO2‐doped Nb3Sn on stainless‐steel samples and as high as 42×106 kOeA/cm2 for CO2‐doped Nb3Sn on Nb samples. For high‐ and medium‐α materials, α is a function of the applied magnetic field; α/αmax vs H/Hc2 is an approximately parabolic function with a maximum value at H/Hc2 = 0.4 for high‐α materials and H/Hc2 = 0.6 for low‐α materials. The latter value is in general agreement with theoretical predictions.