
Hotline:0755-22277778
Tel:0755-22277778
Mobile:13826586185(Mr.Duan)
Fax:0755-22277776
E-mail:duanlian@xianjinyuan.cn
Low permeability absorbing material · Dielectric loss dominant broadband absorbing scheme
In the design of absorbing materials, there is a repeatedly verified rule: the greater the impedance difference between the material and free space, the more difficult it is for electromagnetic waves to enter the interior of the material.
Traditional absorbing materials often use high permeability ferrites or magnetic metal micro powders as absorbers - the higher the permeability, the stronger the ability to "capture" electromagnetic waves. This logic holds in the low frequency range (MHz level): high μ 'efficiently guides magnetic field lines into the interior of the material, and then consumes them through magnetic losses.
But in the high frequency range above GHz, things changed. The magnetic response of high permeability materials rapidly decays with increasing frequency, with a decrease in μ 'and an increase in μ' ', resulting in a sharp decrease in magnetic loss ability. More importantly, high magnetic permeability often means that the material's characteristic impedance is severely mismatched with free space (about 377 Ω). Electromagnetic waves are heavily reflected on the surface of materials and cannot enter at all. How can we talk about absorption?
Core proposition:Low permeability absorbing materials are designed to solve this contradiction. It does not win with "high magnetic permeability", but relies on "good impedance matching" - allowing electromagnetic waves to enter the material first, and then consume them through dielectric loss mechanisms.Advanced Institute of TechnologyThe low magnetic permeability material system is dominated by dielectric loss, with a small amount of magnetic loss synergistic, multiple scattering enhancement, and gradient impedance optimization as the technical route. Under the conditions of μ 'only 1.05-1.80 and μ' ≤ 0.35, the X-band reflection loss is ≤ -20 dB, and the effective absorption bandwidth of Ku/K/Ka band is ≥ 8 GHz.
Impedance matching is a prerequisite for electromagnetic waves to enter the interior of materials. According to the transmission line theory, the normalized input impedance of the material Zin=√ (μ r/ε r) · tanh [j (2 π ft/c) √ (μ r ε r)]. If the surface impedance is severely mismatched with free space, even if the material has strong loss ability, electromagnetic waves will be reflected back at the interface.
Low permeability materials naturally have better impedance matching potential - lower μ 'weakens the magnetic response of the material, equivalent to reducing the overall characteristic impedance of the material, making it closer to the impedance level of free space. But 'potential' does not equal 'reality'. If the dielectric constant is too high, the material impedance will still be mismatched.
Advanced Institute Technology achieves broadband impedance matching through dielectric constant gradient control. The real part of the surface dielectric constant is controlled between 3.5-6.0 (@ 10 GHz), and the imaginary part is controlled between 0.3-0.8, so that the surface reflection coefficient | Gamma |<0.15; The impedance gradient structure of "low dielectric layer high dielectric layer" is formed by increasing the bottom layer ε 'to 15-25 and ε "to 4-8. This gradient design is equivalent to a multi-layer quarter wavelength converter, allowing electromagnetic waves to gradually adapt to impedance changes as they enter the material layer by layer, rather than encountering sudden changes at a single interface. The proportion of frequency bands with vertical incident reflectance better than -12 dB in the range of 8-18 GHz measured by the material exceeds 85%.
Gradient structure designIt is one of the most clever strategies for optimizing impedance matching. By constructing a gradient structure with gradually changing composition, porosity, or conductivity from the surface to the interior, it is possible to achieve a gradual change in wave impedance, making the surface impedance of the material closer to air and reducing initial reflection.
In low permeability materials, the contribution of magnetic loss is relatively limited, and dielectric loss accounts for over 70% of the energy attenuation task. Advanced Institute Technology has activated four types of polarization mechanisms through multi-scale defect engineering to construct a "firepower network" of dielectric loss:
By introducing oxygen-containing functional groups (C=O, C-OH) on the surface of carbon nanotubes/graphene, permanent dipoles are formed. Under the action of an alternating electric field, these dipoles repeatedly flip, converting electromagnetic energy into thermal energy. Its peak value appears at 4-8 GHz, with a peak width exceeding 4 GHz, covering the C-band and some X-band.
Utilizing the core-shell structure Fe ∝ O ₄ @ C SiC@C 、 MXene @ polymer and other heterogeneous interfaces accumulate charges at the interface to form space charge polarization. The interface charge density exceeds 10 ¹⁸ cm ⁻³, the relaxation time is in the range of 10 ⁻⁸ -10 ⁻⁶ s, and its loss contribution is concentrated in 8-26 GHz, covering the X-band to K-band.
Utilize carbon vacancies and nitrogen doped carbon point defects in the silicon carbide lattice to provide losses in the 12-40 GHz frequency range. The defect concentration reaches 10 ¹⁹ -10 ㎡⁰ cm ⁻ ³, allowing the material to maintain effective dielectric loss capability in the millimeter wave frequency band.
By constructing a three-dimensional conductive network and utilizing the migration of electrons within the network to generate Joule heat. SiC/Fe₃ Si@rGO The study of composite aerogels shows that the graphene sheets form a three-dimensional conductive network, and at the same time enhance the conductive loss and interface polarization, so that the materials can achieve effective absorption in the full frequency band of 4 – 18 GHz.
The four types of polarization mechanisms are interconnected in frequency and distributed in different layers of materials in space, collectively forming a dielectric loss system covering 2-40 GHz.
Low magnetic permeability is not equal to zero magnetic permeability. In low permeability materials, although magnetic losses do not dominate, they provide critical supplementary losses in specific frequency bands and participate in fine-tuning impedance matching.
Introduction of Fe ∝ Si phaseIt is a typical case. In SiC/Fe ∝ Si@rGO In the composite aerogel, the Fe ≮ Si phase contributes to the magnetic loss mechanism, which forms a synergistic effect with the conductive loss and interface polarization enhanced by the three-dimensional conductive network of graphene. This multi loss synergy of "dielectric loss as the main and magnetic loss as the auxiliary" enables the material to achieve a minimum reflection loss of -46.68 dB at a thickness of 3.0 mm, and maintain effective absorption in the full frequency range of 4-18 GHz within a thickness range of 1.5-5.0 mm.
In the Ba ∝ Co ₂ Fe ₂₄ O ₄₁ @ CIP composite system, the composite of Co2Z and carbonyl iron powder significantly reduces magnetic and dielectric losses, while minimizing the weakening of magnetic polarization, thereby promoting impedance matching. The resin based patch with a Co2Z: CIP ratio of 1:1 achieved an effective absorption bandwidth of 5.6 GHz (7.4-13 GHz) at a thickness of 1.7 mm, covering the entire X-band.
The core goal of selecting a material system for low permeability absorbing materials is to reduce density while maintaining dielectric loss capability.
Carbon based materials (carbon nanotubes, graphene, carbon fibers)It is the "skeleton" of a low magnetic permeability system. They have high specific surface area, excellent conductivity, and extremely low density, and their dielectric constant can be controlled through defect engineering and surface functional groups. The high conductivity of pure carbon materials can lead to impedance mismatch, so it is necessary to composite with dielectric materials such as SiC to balance electromagnetic parameters.
Silicon carbide (SiC)It is the most widely used ceramic dielectric material in low permeability absorbing materials. SiC nanowires have excellent high-temperature stability and tunable dielectric properties, with carbon vacancies and nitrogen doped defects in their lattice providing effective dielectric losses from 12 GHz to 40 GHz. Advanced Institute Technology combines SiC with carbon materials, utilizing the dielectric loss capability of SiC to complement the conductive loss of carbon materials.
MXeneAs a two-dimensional transition metal carbide/nitride with high conductivity and abundant surface functional groups, it is an ideal material for constructing interface polarization and conductive loss networks. In low permeability systems, MXene is usually used in combination with other materials to regulate the dielectric constant by controlling the filling amount.
Lightweight advantages:The density of low permeability absorbing materials can be as low as 0.9-1.6 g/cm ³, far lower than traditional ferrite absorbing materials (>3.5 g/cm ³), which is crucial for the weight reduction needs of aerospace and portable electronic devices.
When engineers choose low permeability absorbing materials, the following dimensions deserve special attention:
The XJY-D series of low magnetic permeability absorbing materials from Advanced Institute Technology is mainly based on dielectric loss, with a small amount of magnetic loss synergistic as the technical route. The main parameters are as follows:
| performance metrics | XJY-D100 | XJY-D150 | XJY-D200 |
|---|---|---|---|
| Magnetic permeability real part μ ' | 1.05–1.30 | 1.30–1.55 | 1.55–1.80 |
| The imaginary part of magnetic permeability μ " | ≤0.20 | ≤0.28 | ≤0.35 |
| Real part of dielectric constant ε '(@ 10GHz) | 4.5–6.0 | 5.5–7.5 | 7.0–9.5 |
| Reflection loss (X-band) | ≤−18 dB | ≤−20 dB | ≤−22 dB |
| Effective absorption bandwidth (RL ≤ -10dB) | ≥6 GHz | ≥8 GHz | ≥8 GHz |
| thickness range | 0.5–2.0 mm | 0.4–1.5 mm | 0.3–1.2 mm |
| Density | 0.9–1.2 g/cm³ | 1.1–1.4 g/cm³ | 1.3–1.6 g/cm³ |
| Operating Temperature | -40~ 150℃ | -40~ 150℃ | -40~ 150℃ |
| Flame retardant rating | UL94 V-0 | UL94 V-0 | UL94 V-0 |
Data Source:Advanced Institute of Technology
The XJY-D series products support precision die-cutting and adhesive bonding, and can customize thickness, size, and surface treatment methods according to customer needs. The material is suitable for electromagnetic interference suppression in 5G communication equipment, millimeter wave radar, EMC stealth, and precision electronic devices.
The essence of low permeability absorbing materials is an engineering choice made under the physical constraints of high-frequency electromagnetic absorption - not pursuing the maximization of the single indicator of "high permeability", but finding the optimal solution between impedance matching, dielectric loss, density, and thickness. It uses dielectric loss instead of magnetic loss as the main mechanism, uses gradient impedance matching to ensure that electromagnetic waves can enter, uses multi polarization synergy to ensure that electromagnetic waves can be retained and consumed, and uses lightweight material systems to ensure that they are usable.
The evolution of materials from ferrite to carbon based/ceramic based composite systems reflects the upgrade of absorption demand from "MHz level applicability" to "millimeter wave broadband stability". Understanding the engineering relationship between μ 'and impedance matching, the multi polarization synergistic mechanism of dielectric loss, and the trade-off between density and absorption performance - these are the key to upgrading low permeability absorbing materials from "functional materials" to "engineering decisions".
www.avanzado.cn
© 2026 Xianjin Yuan · Technical Reference for Low Magnetic Permeability Absorbing Materials
Advanced Institute (Shenzhen) Technology Co., Ltd, © two thousand and twenty-onewww.xianjinyuan.cn. All Rights Reserved.Guangdong ICP No. 2021051947 sitemap