2022
DOI: 10.1007/s11082-022-03671-2
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Design and optimization of micro-sized wideband fractal MIMO antenna based on characteristic analysis of graphene for terahertz applications

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Cited by 52 publications
(14 citation statements)
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“…Rep 2020 [ 23 ] 0.152 (0.276–0.711 THz) 88.14 4.3 2.58 15 J. Comput. Electron 2022 [ 27 ] 0.353 (0.38–0.42 THz) 10 7 1.1 88 Optik 2020 [ 28 ] 0.245 (0.35–0.75 THz) 72.72 4 2.14 87 Opt. Quantum.…”
Section: Analysis and Discussion On The Resultsmentioning
confidence: 99%
“…Rep 2020 [ 23 ] 0.152 (0.276–0.711 THz) 88.14 4.3 2.58 15 J. Comput. Electron 2022 [ 27 ] 0.353 (0.38–0.42 THz) 10 7 1.1 88 Optik 2020 [ 28 ] 0.245 (0.35–0.75 THz) 72.72 4 2.14 87 Opt. Quantum.…”
Section: Analysis and Discussion On The Resultsmentioning
confidence: 99%
“…In equation ( 1), e 0 and w P are free space permittivity and plasma frequency, respectively. The relaxation time (τ) is 1 × 10 −12 s at room temperature (T) = 100 K [11]. Graphene also provides an important significance as an absorber because it has a very high absorption rate in comparison to radiation in a lower THz frequency regime i.e.…”
Section: Geometrical Layout Of Designed Absorbermentioning
confidence: 99%
“…It supports wideband absorption i.e. 2.37-3.45 THz with more than 90% absorption [11]. Qi et al designed graphene-dielectric based dual band absorber.…”
Section: Introductionmentioning
confidence: 99%
“…It can be seen that the amount of change of θ k (t) at the rise and decay process is 0 from (9), which means θ k (t) behaves as a period of Δt r or Δt f time delay at the rise and decay process, and the change of phase within a T RB is no longer ±π/2. As shown in Figure 6, if Δt r ≠ Δt f , the phase error increases continuously with the accumulation of time, and if the control strategy is adopted, i.e., Δt r � Δt f , the phase error generated in the previous rise/decay process will be compensated in the next rise/decay process, and there is no longer a cumulative error.…”
Section: Effect Of Rotational Motion On Phasementioning
confidence: 99%
“…However, the low-frequency electromagnetic transmitting antennas of existing technologies are all electrically small antennas (ESAs), which rely on the oscillating current in the conductor to excite electromagnetic waves. ere is a Chu-Harrington limit [5][6][7][8][9], making its transmitting system to have features of bulky size, low radiation e ciency, high transmitting power, and energy consumption, which restricts the development of low-frequency electromagnetic communication in related elds.…”
Section: Introductionmentioning
confidence: 99%