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This paper presents a polarization-insensitive rasorber implemented with absorption-transmission-absorption (ATA) characteristics over three consecutive frequency ranges in the terahertz (THz) band. The proposed rasorber is made of a two-layer periodic structure. These two layers are separated by a spacer made of glass substrate. The unit cells of the top layer have a modified swastika geometry metallization, which is loaded with graphene strips to make it lossy and provide dual-band absorption. In the bottom plane frequency selective surface (FSS), a square ring is engraved on the metal layer to obtain bandpass characteristics between two stopbands provided by the top layer. The designed rasorber works in the 0.2 – 1.2 THz frequency range. It provides wideband absorption with a S 11 < − 10 dB from 0.274 to 1.094 THz with a fractional bandwidth (BW) of around 118 % . An in-band transmission window is designed with a S 21 > − 3 dB in the frequency of 0.615 to 0.719 THz provides a large BW of 104 GHz ( 15.59 % ) for THz communication. Within this transmission band, the lowest insertion loss of 0.27 dB is obtained at 0.686 THz. It provides the absorption of more than 80 % in both the lower band ( 0.276 – 0.442 THz, 46.24 % BW) and the higher band ( 0.861 – 1.094 THz, 23.83 % BW). The simulated response of the designed rasorber using a full-wave electromagnetic simulator and calculated through ECM are found to be in good agreement.
This paper presents a polarization-insensitive rasorber implemented with absorption-transmission-absorption (ATA) characteristics over three consecutive frequency ranges in the terahertz (THz) band. The proposed rasorber is made of a two-layer periodic structure. These two layers are separated by a spacer made of glass substrate. The unit cells of the top layer have a modified swastika geometry metallization, which is loaded with graphene strips to make it lossy and provide dual-band absorption. In the bottom plane frequency selective surface (FSS), a square ring is engraved on the metal layer to obtain bandpass characteristics between two stopbands provided by the top layer. The designed rasorber works in the 0.2 – 1.2 THz frequency range. It provides wideband absorption with a S 11 < − 10 dB from 0.274 to 1.094 THz with a fractional bandwidth (BW) of around 118 % . An in-band transmission window is designed with a S 21 > − 3 dB in the frequency of 0.615 to 0.719 THz provides a large BW of 104 GHz ( 15.59 % ) for THz communication. Within this transmission band, the lowest insertion loss of 0.27 dB is obtained at 0.686 THz. It provides the absorption of more than 80 % in both the lower band ( 0.276 – 0.442 THz, 46.24 % BW) and the higher band ( 0.861 – 1.094 THz, 23.83 % BW). The simulated response of the designed rasorber using a full-wave electromagnetic simulator and calculated through ECM are found to be in good agreement.
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