I. Introduction
Circularly polarized (CP) antennas are currently widely used for satellite communication systems. They provide various advantages over linearly polarized (LP) antennas such as multi-path effects, impact due to Faraday rotation, and flexible orientation of transmitting and receiving antennas. A plethora of literature is available on various circularly polarized antennas. Conventionally, patch antennas with slight perturbations fed at a single point such as corner truncated, nearly square antennas [1]–[3] are used for wireless communications due to their compactness and simplicity. Another conventional approach is to generate two orthogonal modes by dual feeding and providing 90° phase shift by using either hybrid or Wilkinson power divider with line is the wavelength at the operating frequency) to generate the additional 90° phase difference on one of its arm. Multi-feeding mechanisms are also reported in the literature. However, these antennas exhibit narrow Axial-Ratio (AR) bandwidth. Although currently widely used for satellite communication systems multi resonators and complex feeding structure [4]. Also, the sequential arrangement of circularly polarized and linearly polarized antennas is used to improve CP radiation for wider bandwidth at the cost of a larger form factor [5]. Quadrifilar helix antennas generate a wide-beam CP pattern and have a larger profile as compared to the planar antennas [6].