and manipulate light. With the crystallization of this new technology, further applications have originated in radar and satellite communications [4; 5], sensing applications [6; 7], microwave and terahertz absorber [8; 9; 10; 11], superlens [12], cloaking devices [13; 14], seismic protection [15], and specific absorption rate (SAR) detection [16; 17]. A double negative (DNG) metamaterial was proposed in [18] based on the modified split H-shape that exhibits single resonance frequency of 6.296 GHz and an EMR of 6.7 fabricated on Rogers RO 3010 substrate material. In [19], an epsilon negative (ENG) metamaterial based on crossed line SRR printed on Rogers RT 5880 dielectric material was introduced that presents triple band resonance frequency covering C-, X- and Ku-band microwave applications. This metamaterial's unit cell size is 10 \(\times\) 10 mm\({}^{2}\) and an EMR of 4.5. In [20], a double C shaped metamaterial for microwave applications was introduced that displays four resonance frequencies at 2.37, 6.12, 8.16, and 14.51 GHz. This metamaterial shows a good EMR of 10.55. A DNG metamaterial based on modified Z-shaped was presented in [21] that is suitable for wideband microwave applications, showing a dual resonance frequency at 7.32 GHz and 11.84 GHz with poor EMR of 4.09. In [22], a DNG metamaterial was proposed based on double C shape that exhibits multiband resonance covering S-, C-, and X- band with EMR of 7.44. A DNG metamaterial based on the double Z-shape was outlined in [23] that presents a triple resonance frequency at 7.3, 8.1, and 9.4 GHz. This metamaterial unit cell size is 8.5 \(\times\) 8.5 mm\({}^{2}\) showing an EMR of 4.8. The negative permittivity metamaterial based on double dumbbell shaped SRR was suggested in [24], that is fabricated on Rogers RT 6002 substrate material. This metamaterial exhibits five resonance frequency covering the S-, X-, and Ku-bands and also shows an excellent EMR of 11.51. The electrical dimension of this metamaterial is 0.087A \(\times\) 0.087A, where \(\lambda\) is calculated at the first resonance frequency. [PERSON] et al. reported the single negative (SNG) metamaterial structure based on concentric ring crossed lines that employed Ku- and Ka-bands, fabricated on FR-4 substrate with an EMR of 4.44 [25]. In another study [26], a DNG metamaterial with size of 5.5 \(\times\) 5.5 mm\({}^{2}\) was introduced that covered C-band microwave applications. This metamaterial exhibits a moderate EMR of 8. Another study demonstrated a metamaterial cloaking operation based on the epsilon negative, in [27]. This cloaking operates in a C-band microwave region and hides the metal cylinder. A hexagonal split-ring resonator with a coupled aperture is proposed as a microwave absorber in [28]. This structure exhibits a dual resonance frequency at 3.56 GHz and 11.67 GHz that is fabricated on a FR-4 substrate covering C and X-band microwave applications. An EMR of this resonator is 8.4. A triple band double negative metamaterial based on the double L-shape was proposed in [29]. This resonator shows a quadruple resonance frequency at 7.69, 8.47, 13.14, and 12.04 GHz and also presents an EMR of 3.9. In addition, [30] presented a double H-shaped SRR based metamaterial that exhibits quadruple resonance for satellite application. The dimension of the unit cell is 9 \(\times\) 9 mm\({}^{2}\), showing an EMR of 10.75. In other research, a cross-coupled interlinked based negative permittivity metamaterial was introduced in [31]. This metamaterial displayed triple resonance at 4.15 GHz, 10.38 GHz, and 14.93 GHz that also shows an EMR of 8.03. This work was also validated through the equivalent circuit model and measurement results. The effect of the dielectric properties of biological materials on the propagation of electromagnetic waves was presented in [32]. This work also delineates the technique of implementing the negative permittivity-based metamaterial structure on a microwave applicator that is enhanced by the control of the electromagnetic field in microwave therapy.