The Aslamazov–Larkin conductivity (ALC) in the layered Dirac/Weyl semi-metals is calculated both for Type-I and Type II for different dimensionality and magnetic fields. The ALC strongly depends on the tilt parameter of the dispersion relation cone. While the 3D and 2D the Aslamazov–Larkin conductivity slightly depends on tilt parameter in Type-I phase and increases in the Type-II phase the 1D ALC decreases in Type-I phase up to zero close to border between Type-I and Type-II phases. Results are discussed in light of the resent experiments on the layered HfTe${}_5$ Weyl semi-metals. It is concluded the one dimensional AL conductivity well explained the experimental data.

针对不同维度和磁场，计算了 I 型和 II 型层状 Dirac/Weyl 半金属中的 Aslamazov-Larkin 电导率 (ALC)。ALC 强烈依赖于色散关系锥的倾斜参数。虽然 3D 和 2D Aslamazov-Larkin 电导率略微取决于 I 型相中的倾斜参数，并且在 II 型相中增加，但 1D ALC 在 I 型相中降低到接近 I 型和 I 型之间边界的零。二阶段。根据对分层 HfTe 的最新实验讨论结果${}_5$外尔半金属。得出的结论是一维 AL 电导率很好地解释了实验数据。