1. Introduction
The birdcage resonators were created for use in magnetic resonance imaging (MRI) [1]. The resonator consists of two endrings and an even number of legs, which connect the endrings together. There are two basic designs, based on the position of the capacitors: high-pass and low-pass [2]. Recently, birdcage resonators were also proposed for utilization in plasma sources [3]. However, for plasma processing, one might expect long-term operation, with hundreds of watts of transmitted power. While the power was usually delivered in the pulse regime in the field of MRI, the continuous regime is expected within the plasma source. This condition will create thermal stress on all parts of the birdcage resonator. Following the standard design, the inserted capacitors will be the weak points. The dimensions of the resonator are in the range of units or tens of centimeters, but the capacitors are usually delivered in SMD housing. Heat can be better dissipated in designs that rely on distributed capacity.