I. Introduction
With a high critical temperature of 39 K, MgB2 superconductor is one of the most promising materials for applications [1]. However, the current density of un-doped MgB2 is sharply depressed due to poor flux pinning as the magnetic field is increased. From the applications point of view, the effect of carbon (C) doping on the upper critical field and of the MgB2 is critical. Recently, many groups have studied C containing compounds and composites, such as SiC, B4C, and carbon nanotubes (CNTs), finding that they improved the and of MgB2 [2]–[6]. A record high of 29 T and of 37 T have been achieved for nano-SiC doped wire at 4.2 K. However, SiC doped MgB2 has a poor thermal and electrical properties. On the other hand, CNTs have excellent thermal, electrical, and mechanical properties [7]. For example, CNTs can carry current densities up to 109 to 1010Acm−2 and remain stable for extended periods of time. The CNT addition may improve the connectivity between grains. The thermal conductivity for CNTs is about 3000 Wm−1K−1 and could benefit the heat dissipation and thermal stability of the MgB2 wires. In addition, CNTs have axial strength and stiffness, approaching that for ideal C fiber. If aligned, CNTs could improve the mechanical properties of MgB2-CNT composite wire. What is worth noting is that CNT can be used as a C source. In the literature, differences in the reactivity of CNT are attributed to the number or size of CNT open end [8]. In general, as the single walled CNT (SWCNT) have a much smaller diameter compared to multi walled CNTs (MWCNTs), a much larger number of open ends can be introduced in SWCNTs. In our study, therefore, we evaluated the doping effect of SWCNT on MgB2 superconductor. Specifications of SWCNT
SWCNT | |
---|---|
Purity | >90% |
Outer diameter [nm] | 1–2 |
Length | 5–15 |
Impurity components | Amorphous C, Mg, Co, Mo, SiO2 |
High resolution transmission electron microscope (HRTEM) image of SWCNTs. The SWCNTs were assembled into bundles. The diameter of each SWCNT ranged from 0.9 to 1.8 nm.