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Materials Science in Additive Manufacturing               Sunflower-inspired microwave-absorbing metastructure




                         A                                  B
















                         C                                   D


















            Figure 8. Effects of individual layer thickness on the absorption performance of the sunflower-inspired metastructure: (A) h , (B) h , (C) h , and (D) h
                                                                                           1   2    3      4
            Figure 9. For effective absorption, Z  should closely match
                                        eff
            the impedance of free space, i.e., the real part should be
            close to 1, and the imaginary part close to 0. This condition
            is generally met above 3.93 GHz. However, in the 2 – 3.93
            GHz range, both the real and imaginary parts fluctuate,
            indicating impedance mismatch and reduced absorption
            efficiency at low frequencies.
              To further explore the metastructure’s angular and
            polarization stabilities, RL was simulated under varying
            incident angles for both transverse electric (TE) and
            transverse magnetic (TM) polarizations. As shown in
            Figure 10, the metastructure maintains robust absorption
            performance across a range of incident angles. Under
            TE polarization, the EAB (RL < −10 dB) remains nearly
            unchanged up to 33°, due to enhanced multiple reflections
            and edge scattering between adjacent units. 34,35  Beyond
            33°, the bandwidth gradually decreases as more waves   Figure 9. Real (Z ’) and imaginary (Z ’’) parts of the equivalent input
            are reflected at higher incident angles. TM polarization   impedance (Z ) for the sunflower-inspired metastructure as a function of
                                                                          eff
                                                                                        eff
                                                                        eff
            demonstrates greater angular stability. Even at 50°, the   frequency, illustrating the impedance matching behavior with free space
            EABs for TE and TM waves remain as high as 10.63 GHz
            and 13.70 GHz, respectively. The centrosymmetric design
            of the metastructure unit also ensures polarization   To  elucidate  the  absorption  mechanisms,  electric
            insensitivity, as confirmed by the consistent response at   and magnetic field distributions were simulated at four
            various polarization angles ranging from 0° (TE mode) to   characteristic peak frequencies: 4.66 GHz, 8.80 GHz,
            90° (TM mode) in Figure 11.                        13.25 GHz, and 17.04 GHz (Figure  12). At the first


            Volume 4 Issue 3 (2025)                         8                         doi: 10.36922/MSAM025220048
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