I. Introduction
Helicon plasma has several outstanding features, notably, the high ionization ratio. It could form a high plasma density of up to m−3, with only a few tens of kilowatts of external radio frequency (RF) power [1]. Besides, the required confinement magnetic field and the aspect ratio of the device are very flexible, making the helicon a very useful plasma source in various applications, e.g., material surface processing and coating, integrated circuit etching, electrode-free plasma thruster, and wall cleaning in tokamaks. In contrast to numerous small-scale helicon devices [2], [3], [4], [5], [6]; nowadays, coupling to large-volume helicon plasmas has attracted more and more attention in multiple research fields [6], [7], [8], [9].