Fig. 1. Electrical transport measurement system in pulsed high magnetic field.脉冲强磁场电输运测量系统

Fig. 2. Rotation sample rod in: (a) Steady-state strong magnetic field; (b) NHMFL (National High Magnetic Field Laboratory).国内外已有转角样品杆　(a) 稳态强磁场中使用的探测样品杆; (b) 美国国家脉冲强磁场中心样品杆

Fig. 3. Rotation sample rod in WHMFC (Wuhan National High Magnetic Field Center): (a) Mechanical structure diagram; (b) situation at different angles; (c) principle of angle calibration.武汉强磁场中心转角样品杆　(a)机械结构图; (b) 转角示意图; (c) 角度标定原理图

Fig. 4. Physical diagram rotation sample rod: (a) Top part; (b) the front of the bottom sample stage; (c) the back of the bottom sample stage.转角样品测量杆实物图　(a) 杆件顶部旋钮及引线罗盘; (b) 底部样品台正面; (c) 底部样品台背面

Fig. 5. Signal processing of angular-dependent electrical transport experiment in 60 T pulsed high magnetic field.60 T脉冲强磁场下转角电输运实验相关数据处理过程

Fig. 6. 3D nested anisotropic Fermi surface construction of Cd₃As₂: (a) Largest cross section of Fermi surface versus the magnetic field orientation; (b) quantum oscillation for B_[112] direction. Cd₃As₂三维嵌套各向异性费米面构造图　(a) 不同晶轴方向的费米面最大横截面; (b) B_[112]方向上的量子振荡

Fig. 7. 2D surface state of a topological insulator Bi₂Se₃: (a) Quantum oscillation^[31]; (b) frequency of the oscillations as a function of θ^[32]. 拓扑绝缘体Bi₂Se₃二维表面态特征　(a) 量子振荡现象^[31]; (b) 振荡频率随转角的变化曲线^[32]

Fig. 8. Quantum limit electrical transport of semi-metal materials in pulsed high magnetic fields: (a) TaP; (b) Bi.脉冲强磁场下的半金属材料量子极限输运研究　(a) TaP; (b) Bi

Fig. 9. Electrical transport of the superconducting material K₂Cr₃As₃: (a) The maximum value of the upper critical field (H_c2) at π/2 indicates the absence the Pauli paramagnetic effect; (b) the polar map of H_c2 shows a unique three fold modulation. 超导材料K₂Cr₃As₃的转角电输运实验结果　(a) π/2处出现上方临界场(H_c2)的最大值表明了泡利极限的缺失; (b) 极坐标图则体现了H_c2的三重调制性