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Fig 1.

Diagram of the structural design and incident field directions for a perfect absorber.

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Fig 2.

Recommended designs for a perfect absorber: (a) Model 1, (b) Model 2, and (c) Model 4 (proposed biosensor design).

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Table 1.

A complete list of the variables that have been adjusted for the recommended sensor.

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Table 1 Expand

Fig 3.

Comparison of the absorption characteristics for different designs: (a) Model 1, and (b) Model 2.

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Fig 4.

Comparison of absorption properties for various designs: (a) Model 3, and (b) Model 4.

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Fig 5.

Comparison of absorption properties for various designs: (a) Model 5, and (b) Model 6.

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Fig 6.

Absorption spectra for the proposed design under varying conditions: (a) substrate material, and (b) resonator material.

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Fig 7.

(a) S11 real and imaginary parts, (b) Reflection and absorption spectra of the absorber.

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Fig 8.

Real and imaginary components of Permeability (μ) and Permittivity (ε) for the proposed absorber: (a) Real components of μ and ε, (b) Imaginary components of μ and ε.

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Fig 9.

Simulated parameter responses of the proposed model: (a) Impedance (z), (b) Real and imaginary parts of the Refractive Index.

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Fig 10.

Visualization of the /E/-field distributions in the metamaterial structure at 0.6408 THz: (a) Real components, (b) Imaginary components.

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Fig 11.

Visualization of the /E/-field distributions in the metamaterial structure at 0.8365 THz: (a) Real components, (b) Imaginary components.

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Fig 12.

Visualization of the /E/-field distributions in the metamaterial structure at 0.965 THz: (a) Real components, (b) Imaginary components.

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Fig 13.

Visualization of the /E/-field distributions in the metamaterial structure at 1.0865 THz: (a) Real components, (b) Imaginary components.

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Fig 14.

Visualization of the /E/-field distributions in the metamaterial structure at 1.195 THz: (a) Real components, (b) Imaginary components.

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Fig 15.

Visualization of the /H/-field distributions in the metamaterial structure at 0.6408 THz: (a) Real components, (b) Imaginary components.

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Fig 16.

Visualization of the /H/-field distributions in the metamaterial structure at 0.8365 THz: (a) Real components, (b) Imaginary components.

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Fig 16 Expand

Fig 17.

Visualization of the /H/-field distributions in the metamaterial structure at 0.965 THz: (a) Real components, (b) Imaginary components.

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Fig 17 Expand

Fig 18.

Visualization of the /H/-field distributions in the metamaterial structure at 1.0865 THz: (a) Real components, (b) Imaginary components.

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Fig 18 Expand

Fig 19.

Visualization of the /H/-field distributions in the metamaterial structure at 1.195 THz: (a) Real components, (b) Imaginary components.

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Fig 19 Expand

Fig 20.

Visualization of the surface current distributions in the metamaterial structure at 0.6408 THz: (a) Real components, (b) Imaginary components.

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Fig 21.

Visualization of the surface current distributions in the metamaterial structure at 0.8365 THz: (a) Real components, (b) Imaginary components.

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Fig 21 Expand

Fig 22.

Visualization of the surface current distributions in the metamaterial structure at 0.965 THz: (a) Real components, (b) Imaginary components.

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Fig 22 Expand

Fig 23.

Visualization of the surface current distributions in the metamaterial structure at 1.0865 THz: (a) Real components, (b) Imaginary components.

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Fig 23 Expand

Fig 24.

Visualization of the surface current distributions in the metamaterial structure at 1.195 THz: (a) Real components, (b) Imaginary components.

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Fig 25.

Analysis of the absorption coefficient of the proposed biosensor in both healthy blood and blood affected by cancer.

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Fig 26.

Detection of absorption coefficients by the proposed biosensor for normal blood and blood cancer within the frequency range of: (a) 0–1.2 THz, (b) 0.6–0.63 THz.

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Fig 27.

Detection of absorption coefficients by the proposed biosensor for normal blood and blood cancer within the frequency range of: (a) 0–1.2 THz, (b) 0.76–0.82 THz.

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Fig 28.

Detection of absorption coefficients by the proposed biosensor for normal blood and blood cancer within the frequency range of: (a) 0–1.2 THz, (b) 1.12–1.20 THz.

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Fig 29.

Utilization of the MWI approach for diagnosing blood cancer.

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Fig 30.

E-field results of the MWI technique: (a) Normal blood, and (b) Blood cancer.

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Fig 31.

H-field results of the MWI technique: (a) Normal blood, and (b) Blood cancer.

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Table 2.

Bio-sensing performance comparisons of various sensor applications based on metamaterial.

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Table 2 Expand

Table 3.

A comparative analysis of terahertz band metamaterial studies and the proposed biosensor design.

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Table 3 Expand