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In situ regulation of microstructure and microwave-absorbing properties of FeSiAl through HNO3 oxidation

  • Yang Guo , Liwen Zhang EMAIL logo , Haipeng Lu EMAIL logo and Xian Jian
Published/Copyright: December 21, 2021
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Abstract

Wrapping insulation of coatings is effective for enhancing the microwave-absorbing properties (MAPs) of ferromagnetic absorbents (FMAs). However, the process is still limited by the low bonding strength with the matrix. Herein, an in situ regulation strategy based on the preparation of thin thickness and strong adhesion insulating layers through HNO3 oxidation was developed to address the limitations. The oxidation process of FeSiAl (FSA) powders was carried out by HNO3 following three main steps. First, the original oxide layer first reacted with HNO3 to form Fe3+ and Al3+. Second, the oxide layer composed of Al2O3 and Fe3O4 was preferentially formed due to the negative change in Gibbs free energy. Finally, the oxide and pigment-deposition layers were subjected to competitive growth and dissolution accompanied by the dissolution of Fe and Al atoms. Oxidation time up to 10 min resulted in the formation of a bilayer structure with a thickness of ∼50 nm on the FSA surface, as well as an outer layer crammed of Al(OH)3 and Fe(OH)3, and an inner layer containing mixed Fe2O3, Fe3O4, Al2O3, and SiO2. The MAPs of as-treated FSA achieved minimum reflection loss (RL) of −25.90 dB at 13.36 GHz, as well as absorption bandwidth of 5.61 GHz (RL < −10 dB) at 10.13–15.74 GHz and thickness of 2.5 mm. In sum, the developed route looks promising for the preparation of high-performance FMAs.

1 Introduction

Advances in the high-speed development of electronic devices and systems led to serious electromagnetic pollution, which attracted increasing attention for the development of high-performance microwave absorbents (MAs) with less pollution [1,2,3,4]. This can be achieved by improving the properties of MAs, especially the reflection loss (RL) value and absorption bandwidth (ABW) below −10 dB through adjustment of composition and/or microstructure [5,6,7,8]. Most methods used for improving microwave-absorbing properties (MAPs) are based on rising the impedance matching degree (Δ) and attenuation constant (a) for electromagnetic wave (EMW) [9,10,11]. For ferromagnetic absorbents (FMAs; Fe, CoNi, and FeNi, etc.), playing an important role in MAs, one way to solve such issues lies in the preparation of thin insulation layers with high resistivity and strong bonding to FMAs [12,13].

In this regard, although organic layers provide desirable bonding strengths, they still suffer from poor resistance in high-temperature treatment (>200°C). This greatly restrains the posttreatment processing temperature [14], thereby reorienting the focus of research to inorganic insulating coatings with good thermal stability [15,16,17,18]. Common inorganic coatings include SiO2 [19], Al2O3 [20], ZnO [21], and MnO2 [22] prepared via hydrothermal reaction and sol–gel method. For hierarchical CoNi@SiO2@C structure, SiO2 and carbon layers could endow CoNi with improved absorbing capability [19]. In this case, RLmin value could reach −46.0 dB at 10.8 GHz, and ABW value may attain 5.6 GHz for film thickness of 2.2 mm. The reason for this has been attributed to the cladding layer enriching the polarization intensity (interface polarization and dipolar relaxation), leading to improved Δ. However, dual-oxide shell ZnO/Al2O3 prepared atomic layer deposition technique showed enhanced MAP of FeSiAl (FSA), thereby can be used as a strong barrier to improve the corrosion resistance [12]. However, the complex and high-cost process would inhibit the commercialization of these methods. In addition, the above processes used for preparing insulating layers suffer from low bonding strength with the matrix. For instance, although SiO2@Al2O3 layer in situ prepared by plasma-induced process is characterized by good bonding strength [23], further optimization in cost control and equipment simplification is required.

Herein, an alternative method involving a direct reaction of microwave absorber with HNO3 to form a surface insulating layer was proposed. To this end, FSA powders were first oxidized by 20 wt% HNO3 at different reaction times. Next, a bilayer structure with a thickness of ∼50 nm was formed at an oxidation time of 10 min, along with an outer layer crammed of Al(OH)3 and Fe(OH)3, as well as an inner layer containing mixed Fe2O3, Fe3O4, Al2O3, and SiO2 grown on the FSA surface. Field-emission scanning electron microscopy (FESEM) and X-ray photoelectron spectroscopy (XPS) analyses provided sufficient information about the morphology and elemental distribution of the oxidation layers, as well as the evolution and growth mechanism of oxide layers. The insulating layers raised the MAP of FSA, with RLmin reaching −25.90 dB at 13.36 GHz and ABW attaining 5.61 GHz at 10.13–15.74 GHz for the film thickness of 2.5 mm. FSA with good “Δ” and strong “a” was achieved by tuning the HNO3 oxidation time, providing a reference for the preparation of other high-performance FMAs.

2 Experimental

2.1 Materials

FSA powders (9.6 wt% Si, 5.4 wt% Al, and 85 wt% Fe) with a mean particle diameter of 45 μm were obtained from Changsha Hualiu Metallurgy Powder Co., Ltd. (Changsha) (AR 99.9%). The preparation process was based on an atomization method.

2.2 Sample synthesis

The materials were prepared by dispersing FSA powders (10 g) in HNO3-ethanol solution (20 wt%, 30 mL) under constant stirring at different oxidation times (1, 5, 10, 20, and 30 min). The resulting suspensions were then filtered and dried at 80°C to yield FSA1NA, FSA5NA, FSA10NA, FSA20NA, and FSA30NA, respectively.

2.3 Characterization

The surface morphologies of the samples were viewed by FESEM (JEOL 7600F, Japan Electronics). X-ray diffraction (XRD, XRD-7000, Shimadzu) at the scanning rate of 2°/min and 2θ of 10–90° was used to investigate the changes in the composition of all samples. The microstructure and composition details of FSA10NA were collected on transmission electron microscopy (TEM, FEI Talos F200x). The XPS data of oxidized coatings were recorded on Escalab 220i spectrometer (VG Scientific) with a monochromatic Al-Kα (1486.7 eV) radiation at 200 W working power. The static magnetic parameters of all samples were collected by vibrating sample magnetometry (cryogen-free magnet-9) mounted on an integrated physical property measurement system. The complex permittivity (ε r ) and permeability (μ r ) of FSA-based composites were obtained by a PNA-L Vector Network Analyzer (type-N5230A, Agilent) at frequencies of 0.5–18 GHz. FSA-based composites were made of FSA and paraffin at a mass ratio of 4:1. The power flow and power loss density were calculated through computer simulation technology (CST) using measured electromagnetic parameters as dielectric and magnetic dispersions. The simulation model was composed of ten lamina with a thickness of 0.25 mm and incident EMWs generated along the opposite Z-direction.

3 Results and discussion

In this study, FSA powders were subjected to a chemical method. Typically, 10 g of as-purchased FSA powders were homogenized in 20 wt% HNO3 solution and mechanically stirred for 1–30 min. The as-treated FSA samples were then filtered off, subsequently washed with deionized water and ethanol, and finally dried in an oven at 80°C for 24 h. The detailed preparation process is depicted in Figure 1a. The evolution SEM images of the microscopic morphologies of the as-treated FSA samples are summarized in Figure 1(b–g). For untreated FSA, the surface remained relatively smooth, as shown in Figure 1b. At processing time with HNO3 of 1 min (Figure 1c), the FSA exhibited a rough surface. The reason for this may have to do with the surface oxide layer of FSA prepared by atomization process during reaction with HNO3, resulting in an exposed matrix. At a treatment time of 5 min, smooth regions were formed on the FSA surface due to the production of thin oxidation coatings (Figure 1d). Further increase in the processing time to 10 min generated a smooth area (Figure 1e). However, corrosion pits and cracks appeared at oxidation times exceeding 20 min (Figure 1f). The cracks then disappeared and oxide films appeared at oxidation times exceeding 30 min (Figure 1g). The reaction products obtained by oxidation with 20 wt% HNO3 for 10 min were further analyzed by high-resolution TEM (Figure 1(h–j)). As shown in Figure 1h, the thickness of the oxide layer was less than 50 nm. The lattice fringe with a distance of 0.21 nm was consistent with Fe3O4 (Figure 1i), and that with a distance of 0.2 nm corresponded to (020) crystalline plane of Fe2O3 (Figure 1j).

Figure 1 
               (a) Schematic of as-treated FSA powders. SEM images showing the surface appearance of FSA powders oxidized at different periods: (b) 0 min, (c) 1 min, (d) 5 min, (e) 10 min, (f) 20 min, and (g) 30 min. (h) TEM image and corresponding HTEM images (I and j) of corrosion products of FSA10NA.
Figure 1

(a) Schematic of as-treated FSA powders. SEM images showing the surface appearance of FSA powders oxidized at different periods: (b) 0 min, (c) 1 min, (d) 5 min, (e) 10 min, (f) 20 min, and (g) 30 min. (h) TEM image and corresponding HTEM images (I and j) of corrosion products of FSA10NA.

The evolution of the surface composition of as-treated FSA during oxidation was studied by XRD. The diffraction peaks of FSA and Al75Fe25 were detected in Figure S1. All samples showed eight peaks corresponding to FSA (JCPDS no. 45-1206) and Al75Fe25 intermetallic compounds (JCPDS no. 45-1178). Also, no significant differences were noticed in XRD patterns of all samples due to the low contents of corrosion products.

The surface composition evolution of as-treated FSA was investigated by probing the surface composition of as-treated FSA using XPS (Figure 2). For untreated FSA, three prominent peaks were noticed at 706.5 [24], 709.9 [25], and 711.4 eV [26] in the high-resolution Fe 2p spectra (Figure 2a) attributable to the Fe0, Fe2+, and Fe3+, respectively. The rough evaluation of surface Fe2+/Fe3+ ratio (>1:2) indicated the existence of FeO. The high-resolution XPS of Al 2p also confirmed the presence of Al0 (72.1 eV) and Al3+ (74.2 eV; Figure 2b). Furthermore, the high-resolution O 1s XPS spectra exhibited four subpeaks located at 530.1, 530.7, 531.9, and 532.8 eV ascribed to FeO [27], Fe3O4 [28], Al2O3 [29], and SiO2 [30], respectively (Figure 2c). Hence, the surface oxide of FSA was produced during the atomization process.

Figure 2 
               High-resolution XPS spectra of (a) Fe 2p, (b) Al 2p, and (c) O 1s recorded for FSA. High-resolution XPS spectra of (d) Fe 2p, (e) Al 2p, and (f) O 1s recorded for FSA10NA. High-resolution XPS spectra of (g) Fe 2p, (h) Al 2p, and (i) O 1s recorded for FSA20NA.
Figure 2

High-resolution XPS spectra of (a) Fe 2p, (b) Al 2p, and (c) O 1s recorded for FSA. High-resolution XPS spectra of (d) Fe 2p, (e) Al 2p, and (f) O 1s recorded for FSA10NA. High-resolution XPS spectra of (g) Fe 2p, (h) Al 2p, and (i) O 1s recorded for FSA20NA.

After oxidation with 20 wt% HNO3 for 10 min, the oxidation products on the FSA surface changed significantly. As indicated by the marks in Figure 2d, the Fe 2p peak at binding energy of 712.3 eV could be assigned to Fe3+ [31], whereas that at 709.5 eV with a satellite signal at 716.0 eV was characteristic of Fe2+ [32]. In high-resolution Al 2p spectra, an Al3+ peak was detected at 73.7 eV and attributed to Al2O3 [33] (Figure 2e). Five peaks were reasonably fitted in O 1s spectrum of Figure 2f, located at 531.4, 531.9, 532.5, 533.2, and 533.8 eV corresponding to Fe3+ [28], Al3+ [29], Si4+ [30], and OH [34], and organic matter (C–O–H) [35], respectively.

At corrosion time of 20 min, the Fe 2p spectrum presented two peaks at 712.5 eV (Fe3+) [36] and 706.5 eV (Fe0) (Figure 2g). As shown in Figure 2h, the Al 2p spectrum can be fitted into two components at 72.1 eV (Al0) and 74.00 eV (Al3+). The appearance of the zero-valent iron and aluminum indicated exposed substrate after corrosion with 20 wt% HNO3-alcohol solutions for 20 min. The O 1 s spectrum displayed in Figure 2f can be deconvoluted into Al3+ (531.9 eV), Si4+ (532.5 eV), OH (533.2 eV), and organic compound (C–O–H; 533.8 eV).

Thermodynamically, Fe3O4 can further be oxidized into Fe2O3 by HNO3. Both zero-valent Fe and Al in FSA might be oxidized by HNO3. In this case, the change in Gibbs free energy (GFE) of Al showed the most negative value due to high reactivity. During the oxidation process, hydroxides like Al(OH)3 and Fe(OH)3 were generated as sediments and may react with nitric acid. Possible reactions occurring during the oxidation can be summarized as follows:

(1) Fe 3 O 4 + 10 HNO 3 = 3 Fe ( NO 3 ) 3 + NO 2 + 5 H 2 O, Δ r G m θ = 327.34 kJ/mol,

(2) Fe 2 O 3 + HNO 3 = 2 Fe ( NO 3 ) 3 + 3 H 2 O, Δ r G m θ = 565.26 kJ/mol,

(3) Al 2 O 3 + 6 HNO 3 = 2 Al ( NO 3 ) 3 + 3 H 2 O, Δ r G m θ = 284.83 kJ/mol ,

(4) 2 Al + 6 HNO 3 = Al 2 O 3 + 6 NO 2 + 3 H 2 O, Δ r G m θ = 1501.72 kJ/mol,

(5) 3 Fe + 8 HNO 3 = Fe 3 O 4 + 8 NO 2 + 4 H 2 O, Δ r G m θ = 907.96 kJ/mol,

(6) Fe ( OH ) 3 + 3 HNO 3 = Fe ( NO ) 3 + 3 H 2 O, Δ r G m θ = 102.82 kJ/mol, and

(7) Al ( OH ) 3 + 3 HNO 3 = Al ( NO ) 3 + 3 H 2 O, Δ r G m θ = 136.32 kJ/mol .

The evolution of surface corrosion of FSA powders oxidized by 20 wt% HNO3 is illustrated in Figure 3. The evolution process mainly included three stages. For pure FSA, the surface oxide layer contained mixed FeO, Fe3O4, Al2O3, and SiO2 formed initially. At an oxidation time of 1 min (Stage I), the original oxide layer reacted with HNO3 to form Fe3+ and Al3+, and the FSA matrix became exposed. At a reaction time of 5 min (Stage II), the oxide layer composed of Al2O3 and Fe3O4 preferentially formed due to the more negative change in GFE. At an oxidation time of 10 min (Stage III), the oxide and precipitation layer experienced competitive growth and dissolution accompanied by the dissolution of iron and aluminum. An oxidation time up to 10 min resulted in the formation of a bilayer structure composed of an outer layer crammed of Fe(OH)3 and Al(OH)3, with an oxide layer containing mixed Fe2O3, Fe3O4, Al2O3, and SiO2. Also, large numbers of bubbles were generated from the violent exothermic reactions at oxidation reaction exceeding 10 min. Such a phenomenon accelerated the dissolution of the surface oxide layer of FSA. As corrosion time increased to 20 min, the oxidation reaction finished one cycle and started a new one. At an extended reaction time of 20 min (Stage IV), the oxide layer and precipitation layer gradually dissolved, leading to an exposed FSA matrix and a new oxidation round of Al and Fe. The difference in reaction rate resulted in the formation of corrosion pits and cracks on the FSA surface. Note that Stage IV was a repetition of Stage I.

Figure 3 
               Schematic showing the evolution mechanism of surface corrosion products of FSA powders oxidized with 20 wt% HNO3.
Figure 3

Schematic showing the evolution mechanism of surface corrosion products of FSA powders oxidized with 20 wt% HNO3.

The complex ε r and μ r obtained at frequencies of 0.5–18 GHz are summarized in Figure 4. The real part (μ′) and imaginary part (μ″) of μ r deputy the magnetic capacity, the real part (ε′) and imaginary part (ε″) of ε r express the dielectric capability. No significant differences in μ′ and μ″ of μ r were seen for samples oxidized by 20 wt% HNO3 for 1–30 min (Figure 4(a–b)). The ε′ of ε r first increased and then decreased within 1–10 min. Besides, the trend appeared periodically at a reaction time of 10–30 min. The ε′ of FSA5NA increased from 8.9 to 8.2 when compared to FSA, which enhanced from 7.0 to 7.5 (Figure 4c). The increase in 20 wt% HNO3 oxidation time to 10 min led to a decline in ε′ from 8.2 to 7.9. As the oxidation time further increased to 20 min, the ε′ of FSA20NA incremented from 7.9 to 8.7 and then 7.5 to 7.9. Two vibration peaks were observed at ∼10 and ∼14 GHz and could, respectively, be attributed to surface geometric enhancement effect and local space charge accumulation [37,38]. Nevertheless, the ε″ of ε r of as-treated FSA showed an opposite trend when compared to the real part, accompanied by some slight fluctuations (Figure 4d). The changes in ε″ and μ″ demonstrated the dissipation capabilities of the electric and magnetic energies, respectively [39]. In other words, FSA10NA exhibited excellent EMW attenuation and loss ability due to the high ε″ value originating from the oxide layers with unique micro-nano construction features.

Figure 4 
               Frequency dependence of electromagnetic parameters of FSA, FSA1NA, FSA5NA, FSA10NA, FSA20NA, and FSA30NA. (a) Real part and (b) imaginary part of complex permeability. (c) Real part and (d) imaginary part of complex permittivity.
Figure 4

Frequency dependence of electromagnetic parameters of FSA, FSA1NA, FSA5NA, FSA10NA, FSA20NA, and FSA30NA. (a) Real part and (b) imaginary part of complex permeability. (c) Real part and (d) imaginary part of complex permittivity.

The MAP values of all samples were obtained by calculating RL from measured electromagnetic parameters based on transmit line theory that can be expressed by equations (8) and (9) [40,41,42]:

(8) Z in = Z 0 μ r ε r tanh j 2 π f c d μ r ε r ,

(9) RL = 20 lg Z in Z 0 Z in + Z 0 ,

where Z in represents input impedance (Z in), Z 0 is air impedance, f refers to microwave frequency, d denotes absorber thickness, and c is the speed of light.

The three-dimensional (3D) colormaps of FSA, FSA1NA, FSA5NA, FSA10NA, FSA20NA, and FSA30NA obtained by regulating the thickness from 0.5 to 5.0 mm are depicted in Figure 5(a–f). The comparison of RL values at different thicknesses revealed FSA10NA with the strongest MAP. The RL curves of FSA, FSA10NA, and FSA20NA at 0.5–18 GHz and thickness of 2.5 mm are compared in Figure 5g. The RLmin of −25.30, −25.90, and −20.21 dB, as well as ABW of 4.47 GHz (11.29–15.75 GHz), 5.61 GHz (10.13–15.74 GHz), and 4.44 GHz (10.99–17.43 GHz), corresponded to FSA, FSA10NA, and FSA20NA, respectively. The RL curves in Figure S2 exhibited a shift in minimum RL frequency (f min) to lower values as d increased from 0.5 to 5.0 mm. Thus, thicker coatings suppressed the region with narrow reflection frequency. This can be explained by the quarter-wavelength equation:

t m = n λ 4 = n c 4 f m μ r ε r , ( n = 1 , 3 , 5 , ) ,

[43,44,45], where t m presents the thickness of the absorber, λ stands for the wavelength of EMW, f m is the peak frequency of minimum RL, and c refers to the speed of light in vacuum. The comparison suggested enhanced MAP of FSA10NA toward EMW. The reason for this had to do with, first, the oxide layers formed on the FSA surface by nitric acid, which reduced the reflectivity of EMW and provided abundant electron transportation path to hop into the FSA10NA conducive due to loss in electromagnetic waves. Second, the polarization movement also fell behind the change in the alternating electromagnetic field, resulting in a relaxation phenomenon (Figure 5h). According to the Debye relaxation theory [46,47], a single semicircle curve of εversus ε″ would indicate relative materials with strong polarization behavior, where each semicircle would present one Debye relaxation process. Here, FSA, FSA10NA, and FSA20NA exhibited some Cole–Cole semicircles, revealing strong polarization relaxations (Figure S3). Third, FSA10NA had better magnetic properties (122.6 emu/g), favorable to the formation of 3D magnetically connected network, which can catch up with the incident EMW to enhance the magnetic loss ability (Figure S4 and Table S1). In general, the magnetic loss capability induced by the eddy-current effect would primarily be located in the high-frequency region (∼11 GHz) for MAs. Here, the μ ( μ ) 2 ( f ) 1 values of FSA, FSA10NA, and FSA20NA were almost constant at 11–18 GHz (Figure S5), indicating the contribution of eddy-current loss to enhancement in MAP values (Figure 5i).

Figure 5 
               Frequency and thickness dependence of simulated 3D color maps of (a) FSA, (b) FSA1NA, (c) FSA5NA, (d) FSA10NA, (e) FSA20NA, and (f) FSA30NA. (g) RL curves of FSA, FSA1NA, FSA5NA, FSA10NA, FSA20NA, and FSA30NA in 0.5–18 GHz at a thickness of 2.5 mm. Schematic of (h) interfacial polarization, (i) eddy current, and (j) natural resonance in FSA-based 3D net.
Figure 5

Frequency and thickness dependence of simulated 3D color maps of (a) FSA, (b) FSA1NA, (c) FSA5NA, (d) FSA10NA, (e) FSA20NA, and (f) FSA30NA. (g) RL curves of FSA, FSA1NA, FSA5NA, FSA10NA, FSA20NA, and FSA30NA in 0.5–18 GHz at a thickness of 2.5 mm. Schematic of (h) interfacial polarization, (i) eddy current, and (j) natural resonance in FSA-based 3D net.

In general, the loss in capacity of MAs to EMW could be mainly reflected in the balance between Δ and a [48]. A higher a would lead to better dissipation ability for EMW, while a Δ closed to 0 would indicate optimal impedance matching characteristics. The a–f curves of FSA, FSA10NA, and FSA20NA are given in Figure S6. Obviously, the a of FSA10NA showed a rising trend at frequencies of 4–16 GHz, demonstrating an enhanced EMW attenuation ability. Figure 6a displays the Δ–f contour maps of FSA, FSA10NA, and FSA20NA under 0.5–5.0 mm. FSA10NA displayed the optimal Δ values (as blue as possible), showing the beneficial effects after moderate oxidation on MAP.

Figure 6 
               (a) The calculated data maps of FSA, FSA10NA, and FSA20NA at 0.5–18 GHz. (b) Power flow and (c) power loss density distribution images of FSA, FSA10NA, and FSA20NA under 2.5 mm at 13.36 GHz.
Figure 6

(a) The calculated data maps of FSA, FSA10NA, and FSA20NA at 0.5–18 GHz. (b) Power flow and (c) power loss density distribution images of FSA, FSA10NA, and FSA20NA under 2.5 mm at 13.36 GHz.

To further confirm the beneficial effects of moderate oxidation on “a” and “Δ”, the power flow and power loss density distributions of FSA, FSA10NA, and FSA20NA were obtained by CST simulations. To this end, the CST simulation model was confirmed by comparing the S11 parameters with the calculated RL values. As shown in Figure S8, the S11 curves of FSA, FSA10NA, and FSA20NA all agreed with the corresponding calculated RL, indicating the suitability of the simulation method. Based on this simulation model, the power flow density and power loss density were simulated through CST. Note that the power flow density can be obtained by equations (10) and (11) [49]:

(10) S av = 1 T 0 T S d t = 1 2 Re [ E × H ] ,

(11) S = E × H .

According to the arrows marked with different color fills (Figure 6b), the power flow entering the absorbers declined in the following order: FSA10NA > FSA > FSA20NA. This further verified the impedance characteristics of all absorbers demonstrated in Figure 6a. The values of power loss density (W/m3) of FSA, FSA10NA, and FSA20NA under 2.5 mm at 13.36 GHz are displayed in Figure 6c. The values of power loss density of all three absorbers illustrated a revised trend under the same fixed conditions, confirming the gradual EMW consumption inside the absorbers. The comprehensive comparison revealed FSA10NA with optimal attenuation capacity when compared to FSA and FSA20NA. The above CST simulation results proved the importance of balance between “a” and “Δ.”

4 Conclusion

An ultra-thin insulating layer was successfully formed on the FSA surface through HNO3 oxidation. The oxidation process of FSA powders with 20 wt% HNO3 mainly involved three stages. At an oxidation time of 1 min (Stage I), the original oxide layer reacted with HNO3 to form Fe3+ and Al3+, and the FSA matrix was exposed. For oxidation reaction time up to 5 min (Stage II), an oxide layer composed of Al2O3 and Fe3O4 preferentially formed due to the more change in negative GFE. At an oxidation time of 10 min (Stage III), the oxide layer and precipitation layer exhibited competitive growth and dissolution accompanied by the dissolution of iron and aluminum. A bilayer structure with a thickness of ∼50 nm formed with the outer layer composed of Fe(OH)3 and Al(OH)3. The oxide layer contained mixed Fe2O3, Fe3O4, Al2O3, and SiO2. FSA10NA exhibited significantly enhanced MAP with RLmin reaching up to −25.90 dB at 13.36 GHz and ABW attaining up to 5.61 GHz (<−10 dB) at the thickness of 2.5 mm. In sum, the suggested method looks promising for the preparation of high-performance FMAs with stronger RL and wider ABW.

  1. Funding information: The study was supported by funds from the Guiding Science and Technology Plan Project of Panzhihua (2021ZD-G-4), the Open Projects of Vanadium and Titanium Resource Comprehensive Utilization Key Laboratory of Sichuan Province (2021FTSZ05 and 2021FTSZ11), the Open Foundation of National Engineering Research Center of Electromagnetic Radiation Control Materials (ZYGX202K003-1), and the National Natural Science Foundation of China (No. 51972046).

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

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Received: 2021-10-17
Revised: 2021-10-26
Accepted: 2021-10-31
Published Online: 2021-12-21

© 2022 Yang Guo et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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