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Abbreviation (ISO4): Prog Chem      Editor in chief: Jincai ZHAO

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Carbon-Based Composite Absorbing Materials

  • Lu Shuiqing 1, 2, 3 ,
  • Liu Yichang 1, 2, 3 ,
  • Xie Zhipeng 1, 2, 3 ,
  • Zhang Da , 1, 2, 3, * ,
  • Yang Bin 1, 2, 3 ,
  • Liang Feng , 1, 2, 3, *
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  • 1 Key Laboratory for Nonferrous Vacuum Metallurgy of Yunnan Province, Kunming University of Science and Technology, Kunming 650093, China
  • 2 National Engineering Research Center of Vacuum Metallurgy, Kunming University of Science and Technology, Kunming 650093, China
  • 3 Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology, Kunming 650093, China
*e-mail: (Feng Liang);
(Da Zhang)

Received date: 2023-08-15

  Revised date: 2023-11-12

  Online published: 2024-03-15

Supported by

National Natural Science Foundation of China(12175089)

National Natural Science Foundation of China(12205127)

Key Research and Development Program of Yunnan Province(202103AF140006)

Applied Basic Research Programs of Yunnan Provincial Science and Technology Department(202001AW070004)

Applied Basic Research Programs of Yunnan Provincial Science and Technology Department(202301AS070051)

Applied Basic Research Programs of Yunnan Provincial Science and Technology Department(202301AU070064)

Yunnan Industrial Innovative Talents Program for "Xingdian Talent Support Plan"(KKXY202252001)

Yunnan Program for Introducing Foreign Talents(202305AO350042)

Yunnan Major Scientific and Technological Projects(202202AG050003)

Abstract

with the rapid development of radio waves and electronic information technology,the problem of electromagnetic radiation pollution is becoming more and more prominent,which has attracted wide attention around the world.in order to solve the problem of electromagnetic pollution,people are committed to researching and developing electromagnetic wave-absorbing materials with light weight,thin thickness,a wide frequency band,and strong absorption.Compared with traditional wave-absorbing materials,carbon-based composite wave-absorbing materials have excellent dielectric properties,special microstructure,good impedance matching and efficient wave-absorbing properties,and can effectively reduce the mass of composite materials,which has great development potential In the field of wave-absorbing materials,and has gradually become a research hotspot.In this paper,the basic absorption principle of electromagnetic wave is summarized from the aspects of impedance matching and loss mechanism,and the research progress of carbon-carbon,carbon-metal/metal oxide,carbon-ceramics and other kinds of carbon-based composite absorbing materials is reviewed.At the same time,the synthesis methods,absorption properties and attenuation mechanism of these carbon-based composite absorbing materials are reviewed.Finally,the shortcomings of carbon-based composite absorbing materials in electromagnetic wave absorption are discussed and possible solutions are put forward,and the future development direction of carbon-based composite absorbing materials is prospected。

Contents

1 Introduction

2 Absorbing mechanism and classification of absorbing materials

2.1 Absorbing mechanism

2.2 Classification of absorbing materials

3 Carbon nano-absorbing materials

4 Carbon-based composite absorbing materials

4.1 carbon-carbon composite absorbing materials

4.2 Carbon-metal/metal oxide composite absorbing materials

4.3 Carbon-ceramic composite absorbing materials

5 Conclusion and outlook

Cite this article

Lu Shuiqing , Liu Yichang , Xie Zhipeng , Zhang Da , Yang Bin , Liang Feng . Carbon-Based Composite Absorbing Materials[J]. Progress in Chemistry, 2024 , 36(4) : 556 -574 . DOI: 10.7536/PC230814

1 Introduction

As the driving force of scientific and technological revolution,electronic information technology has brought great convenience to national defense and daily life.With the increasing popularity of electronic devices,wireless communication technology inevitably produces a large number of electromagnetic radiation of different frequencies[1]。 In civil and military fields,electromagnetic radiation can cause serious electromagnetic interference between electronic components and endanger human health and national security[2]。 Therefore,electromagnetic pollution has become a key problem to be solved urgently.There are generally two ways to avoid electromagnetic pollution:one is to use electromagnetic shielding materials to reflect electromagnetic waves,and the other is to use electromagnetic wave absorbing materials(absorbing materials)to absorb electromagnetic waves[3][4]。 However,the electromagnetic wave reflected by the former is easy to produce secondary pollution,so Absorbing materials have become the first choice to prevent electromagnetic pollution.absorbing materials refer to a class of functional materials that can absorb and attenuate incident electromagnetic waves,and convert electromagnetic energy into heat energy or other forms of energy to consume or make electromagnetic waves disappear due to interference[5]。 At the same time,the ideal absorbing material should also have the characteristics of"thin,light,wide and strong",and the development of absorbing materials with thin thickness,low density,wide absorption bandwidth and high absorption intensity is the goal pursued by many researchers[6]。 In addition,absorbing materials also need to have excellent mechanical properties,high thermal stability,oxidation resistance,corrosion resistance and other characteristics to meet the needs of complex application scenarios and prolong their service life[7][8]
Traditional microwave absorbing materials such as ferrite,silicon carbide and magnetic metal powder have been widely used[9][10]。 However,they usually have high density,easy oxidation,and narrow effective absorption bandwidth,which seriously limit their practical applications[11]。 Compared with traditional microwave absorbing materials,carbon nanomaterials have multi-dimensional allotropic structures(such as zero-dimensional carbon nanospheres,one-dimensional carbon nanotubes,two-dimensional graphene,three-dimensional porous carbon,etc.),which have broad application prospects in electromagnetic wave absorption due to their high conductivity,high specific surface area,low density and high chemical stability[12][13][14][15][16]。 However,due to the single loss mechanism and high conductivity of single-component carbon nanomaterials,the impedance matching of carbon nanomaterials is not good,and it is difficult to achieve good microwave absorption effect[17]。 Therefore,in order to solve the above problems,carbon nanomaterials are combined with different materials(carbon,magnetic metals,metal oxides and ceramics)to form carbon-based composite absorbing materials.By improving the dielectric properties of the composite,the magnetic loss mechanism is introduced to enhance the permeability,thereby improving the impedance matching and improving the microwave absorbing properties[18]。 At the same time,the heterogeneous interface is easy to form in the carbon-based composite absorbing materials[19]。 On the one hand,the heterointerface inherits the unique electromagnetic properties of the constituent materials,such as dielectric and magnetic properties,which can maximize the balance of impedance matching and enhance energy dissipation[20]。 On the other hand,the formation of heterointerface can change the band alignment,space charge,electron transport,lattice defects,lattice strain and other characteristics of carbon-based composite absorbing materials[21]。 These properties have a fundamental impact on the dipole polarization,interface polarization,conduction loss and magnetic response,and help to improve the absorbing properties of carbon-based composite materials[22]
In this paper,the research progress of carbon-based composite absorbing materials is reviewed based on the recent research situation at home and abroad.the synthesis methods,morphology and absorbing properties of the composite absorbing materials are described,and the absorbing mechanism is summarized.Finally,the challenges and problems of radar absorbing materials are put forward,and the future development of radar absorbing materials is prospected。

2 Microwave Absorbing Mechanism and Classification of Microwave Absorbing Materials

When the electromagnetic wave reaches the surface of the material,the incident wave,the reflected wave,and the transmitted wave are generated,as shown in Figure 1(a).An ideal absorber should absorb the incident wave and reduce the generation of reflected and transmitted waves as much as possible,as shown in Fig.1(B).At the same time,the absorbing material should also have low interface impedance and high attenuation characteristics[23]。 Among them,low interface impedance means that the material has weak reflection of electromagnetic waves,and the electromagnetic waves can enter the material to the maximum extent.High attenuation characteristics indicate that the material has a strong ability to attenuate electromagnetic waves and can quickly convert electromagnetic energy into heat or other forms of energy[24]。 in addition,the electromagnetic wave In the material produces destructive interference due to inhomogeneous scattering,that is,when the incident wave and the reflected wave differ by 1/4 wavelength and their phase difference is 180°,the two waves will attenuate each other's energy through destructive interference[25]。 In addition,The strength of the electromagnetic wave absorbed by the absorbing material can be expressed by the peak value of the reflection loss.the peak value of reflection loss is calculated by equations(1~4):[26]
$ R_{L}=20 \lg \left|\frac{z_{i n}-z_{0}}{z_{i n}+z_{0}}\right|$
$ Z_{i n}=Z_{0}\left(\frac{\mu_{r}}{\varepsilon_{r}}\right)^{\frac{1}{2}} \tan h\left[j\left(\frac{2 \pi f d}{c}\right)\left(\mu_{r} \varepsilon_{r}\right)^{\frac{1}{2}}\right]$
$ \varepsilon_{r}=\varepsilon^{\prime}-j \varepsilon^{\prime \prime}$
$ \mu_{r}=\mu^{\prime}-j \mu^{\prime \prime}$
图1 (a) 吸波材料与电磁波相互作用示意图;(b) 理想吸波材料表面对电磁波反射示意图[23]

Fig. 1 Schematic diagram of the (a) Interaction between electromagnetic waves and absorber, (b) Reflection of electromagnetic wave on the surface of ideal absorbing material [23]

The RL(Reflection loss)of the above equation is the reflection loss in dB.Reflection loss is an important index to measure the absorption performance of radar absorbing materials.When the reflection loss reaches-10 dB,it shows that the material can absorb 90%of the electromagnetic wave.When the reflection loss reaches-20 dB,it indicates that the material can absorb 99%of the electromagnetic wave.The larger the absolute value of the RLis,the better the absorbing performance of the material is.The frequency range exceeding-10 dB is called the effective absorption bandwidth.Zinis the impedance of the incident wave in free space and at the interface,in units ofΩ;Z0is the impedance of the incident wave in free space,in units ofΩ;εrandμrare the relative complex permittivity and relative complex permeability of the material,respectively,where the real part(ε',μ')represents the electric energy storage and magnetic energy storage capabilities of the material,and the imaginary part(ε'',μ'')represents the dielectric loss and magnetic loss capabilities of the material for electromagnetic waves;F is the frequency of free space electromagnetic wave;D is the sample thickness;C is the speed of light 。

2.1 Absorbing mechanism

2.1.1 Impedance matching

Impedance matching is a parameter to study the interaction between electromagnetic waves and materials and the effect of wave transmission in different frequency bands.Impedance matching directly affects the radar absorbing properties of materials,which is the prior condition and[27]in the research and development of radar absorbing materials.The Z value is usually used to characterize the impedance matching,as shown in formula(5).The closer the Z value is to 1,the better the impedance matching of the material is.The electromagnetic wave can enter the material to the maximum extent,and the absorbing material can play the greatest role[28]。 On the contrary,it shows that the impedance matching is not good,most of the electromagnetic waves are reflected,and the absorbing performance of the material is poor。
$ Z=\left|\frac{z_{\text {in }}}{z_{0}}\right|$

2.1.2 Dielectric loss

Dielectric loss is the characteristic electron interaction between the electric field and the absorbing material to consume the electromagnetic wave energy,which is mainly caused by the conduction loss and polarization loss[29]。 Dielectric loss factor(tanδε=ε″/ε′)is usually used to characterize the dielectric attenuation ability.The imaginary part is calculated as shown in equation(6 )[30]
The conduction loss(εc")refers to the loss form in which the electric energy is converted into heat energy to be dissipated due to the directional movement of conductive carriers to generate macroscopic current under the action of an applied electric field,as shown in Equation(7 )[31]。 Polarization loss(εp")means that a charged particle will produce an electric dipole moment under the action of an electric field.When the direction of the electromagnetic field changes,the electric dipole moment changes with it.In order to keep synchronization with the electric field,the charged particle needs to vibrate or rotate to produce polarization,resulting in energy loss,which can be understood as the result of the thermal motion of the charged particle driven by overcoming the electric field force,as shown in Equation(8).The main polarization forms are ionic polarization,electronic polarization,dipole polarization and interfacial polarization.Ion polarization and electron polarization only occur in the high frequency region,while dipole polarization and interface polarization mainly occur in the microwave region(2~18 GHz )[32-34]
In addition,when the polarization process of the material can not keep up with the frequency change of the electromagnetic field,the polarization relaxation phenomenon will occur[35]。 the microscopic level means that when the charge in the dielectric is restricted by defects or functional groups,it can not move freely like the electrons in the external electric field,so polarization relaxation occurs.According to the Debye relaxation theory,the relaxation process can be represented by Cole-Cole semicircles,where each semicircle represents a polarization relaxation process[36]。 As shown in equation(9)[37]
$ \varepsilon^{\prime \prime}=\frac{1}{2 \pi \sigma f \varepsilon_{0}}$
$ \varepsilon_{c}^{\prime \prime}=\frac{\sigma}{\omega \varepsilon_{0}}$
$ \varepsilon_{p}^{\prime \prime}=\frac{\omega \tau\left(\varepsilon_{s}-\varepsilon_{\infty}\right)}{1+\omega^{2} \tau^{2}}$
$ \left(\varepsilon^{\prime}-\varepsilon_{\infty}\right)^{2}+\left(\varepsilon^{\prime \prime}\right)^{2}=\left(\varepsilon_{s}-\varepsilon_{\infty}\right)^{2}$
Where f is the electromagnetic wave frequency,is the material resistivity,andε0is the vacuum permittivity.ωdenotes the angular frequency,τis the polarization relaxation time,εsis the static dielectric constant,andεis the relative dielectric constant at infinite frequency 。

2.1.3 Magnetic loss

magnetic loss refers to the loss mechanism in which a part of energy is irreversibly converted into heat and dissipated when a Magnetic material is placed in an electromagnetic field and undergoes magnetization and magnetization reversal processes[38]。 The magnetic loss factor(tanδ′μ=μ″/μ′)is usually used to characterize the magnetic attenuation ability[39]。 the main types of magnetic loss are Hysteresis loss,domain wall resonance,natural resonance,exchange resonance and eddy current loss.hysteresis losses are negligible in weak magnetic fields,and domain wall resonances occur only in The MHz frequency range.The main magnetic losses occurring in the microwave region are natural resonance,exchange resonance,and eddy current losses。
natural resonance is a special form of ferromagnetic resonance.In the absence of an external constant magnetic field,the maximum of relative complex permeability will occur due to the existence of an equivalent field of magnetocrystalline anisotropy,which is called Natural resonance[40]
in ferromagnetic materials,due to the influence of thermal turbulence or other factors,some electron spins contributing to magnetism deviate from the original ordered arrangement direction,and under the interaction of exchange interaction and magnetic dipole moment,These locally deviated spins precess and propagate towards other parts of the ordered body,and this collective motion pattern of spins in the magnetically ordered body is called spin wave.Once the effect of the exchange interaction is much larger than that of the dipolar interaction,the exchange resonance will occur and multiple resonance peaks will be generated.In general,the natural resonance usually occurs in the frequency range of 0.10∼10.0 GHz,while the exchange resonance occurs in the higher frequency range[38,41]
In addition,in order to evaluate the contribution of eddy current loss,the C0is usually used for judgment.If the magnetic loss mainly originates from the eddy current loss,the C0is a constant that does not change with the frequency of the incident electromagnetic wave.As shown in equation(10 )[42]
$ C_{0}=\mu^{\prime \prime}\left(\mu^{\prime}\right)^{-2} f^{-1}$

2.1.4 Attenuation constant

in order to characterize the attenuation degree of electromagnetic wave by absorbing materials,the attenuation constantαis usually used.the attenuation constantαdetermines the dissipative properties of the material,as shown In Equation(11)[43]
$ \alpha=[(\sqrt{2 \pi} f) / c] \cdot\left\{\left(\mu^{\prime \prime} \varepsilon^{\prime \prime}-\mu^{\prime} \varepsilon^{\prime}\right)+\left[\left(\mu^{\prime \prime} \varepsilon^{\prime \prime}-\mu^{\prime} \varepsilon^{\prime}\right)^{2}+\left(\mu^{\prime} \varepsilon^{\prime \prime}+\mu^{\prime \prime} \varepsilon^{\prime}\right)^{2}\right]^{\frac{1}{2}}\right\}^{\frac{1}{2}}$

2.1.5 Quarter-wave cancellation law

the thickness of the absorbing material affects its absorbing performance as well as the production cost.Generally,the thickness of the material and the matching frequency should follow the quarter-wave cancellation law[44]。 When The matching thickness of the material meets 1/4 times of the wavelength or odd times of 1/4,the interference between electromagnetic waves will be cancelled,thus promoting the attenuation of electromagnetic waves.the formula is shown in(12)[45]
$ d_{m}=\frac{n \lambda}{4}=\frac{n c}{4 f_{m} \sqrt{\left|\mu_{r} \| \varepsilon_{r}\right|}}$
dmis the matching thickness of the material,n=1,3,5,…,λis the wavelength of the electromagnetic wave,C is the speed of light,and fmis the matching frequency 。

2.2 Classification of radar absorbing materials

absorbing materials can be divided into conversion type and consumption type according to The action mechanism,and the conversion type is resistance type absorbing materials;the consumptive type is dielectric type absorbing material and magnetic medium type absorbing material[46]。 Resistive absorbing materials mainly include carbon black,carbon fiber,silicon carbide and Graphene(GN),etc.Their absorbing forms are based on conductive loss and dielectric loss.Through the interaction with the external electric field,the incident wave is converted into heat energy to achieve the purpose of absorbing electromagnetic waves.However,according to the free electron theory,too high conductivity is not conducive to impedance matching,resulting in electromagnetic wave reflection on the surface of the material,thus reducing the absorbing performance of the material[47][48]。 dielectric absorbing materials mainly include barium iron titanate ceramics,which absorb electromagnetic waves based on dipole polarization and interface polarization,and produce Dielectric relaxation loss electromagnetic waves in an external electric field[49]。 magnetic dielectric absorbing materials include ferrite,carbonyl iron and metal powder,and their absorbing forms are based on Magnetic loss to consume electromagnetic waves[50]

3 Carbon nanomaterials for radar absorption

GN and carbon nanotubes are popular nano-absorbing materials in recent years.GN was first prepared by mechanical exfoliation in 2004 by Geim and Novoselov et al[51]。 as a hexagonal two-dimensional material composed of carbon atoms,it has many excellent properties,such As the Young's modulus of graphene is 1.0 TPa[52]; Excellent flexibility and mechanical strength;The high thermal conductivity is about 5300 W·m−1·K−1[53];The specific surface area is up to 2630 m2·g−1[54],the carrier mobility at room temperature is up to 15 000 cm2·V−1·s−1[55],etc.At the same time,graphene also has special effects such as quantum tunnel effect and quantum Hall effect[56]。 In terms of electromagnetic wave absorption,graphene has the following advantages:high specific Surface area and high conductivity promote dielectric loss;surface defects and functional groups are easy to produce dipole polarization.the capacitor-like sheet structure is conducive to charge storage,and the multiple reflection and scattering of electromagnetic waves between the sheets are conducive to the dissipation of electromagnetic waves.the good conductive network promotes electron transport and produces resistive loss,and these advantages promote the application of graphene composite absorbing materials[57]。 Wang et al.Studied the microwave absorbing properties of Reduced graphene oxide(Reduced graphene oxide,rGO)[58]。 the surface defects and functional groups of the material increase the polarization of rGO and improve its microwave absorbing properties.When the thickness of rGO is only 2 mm,the peak reflection loss is-6.9 dB at 7 GHz,which is better than that of graphite under the same conditions。
carbon nanotubes(CNTs)are composed of graphite-like hexagonal grids,which are generally divided into Single-walled carbon nanotubes(SWCNTs)and Multi-walled carbon nanotubes(MWCNTs),with diameters ranging from a few nanometers to tens of nanometers and lengths up to microns[59]。 Compared with steel,the elastic modulus of CNTs is 5 times that of steel,the elastic strain is 60 times that of steel,while the density is only 1/6 of steel,and the thermal conductivity is as high as 3000 W·m−1·K−1at room temperature[60]。 In the aspect of electromagnetic wave absorption,the large specific surface area of CNTs improves the interfacial polarization probability[61]; the rich functional groups and defects on the surface promote the dipole polarization[62]; the high porosity promotes the multiple scattering and reflection of electromagnetic waves,which makes CNTs have broad application prospects in the direction of microwave absorption[63]
In addition to the above two materials,researchers also hope to design carbon nanomaterials with high porosity and special microstructure to improve the absorbing properties.Zhao et al.Constructed a SiO2layer on the surface of ZIF-67 microcube,and successfully constructed hollow porous carbon microcube(HPCMC)through high temperature pyrolysis and etching.The special middle cavity structure enables HPCMC to form a conductive network matrix in paraffin and make a significant contribution to conduction loss.The high porosity also ensures a large surface area,which is easy to produce abundant heterogeneous interface polarization[64]。 Cui et al.Successfully fabricated a series of hollow NiCo@C microboxes by alkaline etching,in situ conversion,and phenolic resin(PR)reinforcement using nickel cobalt Prussian blue analogue microcubes as precursors[65]。 the unique hollow microstructure with large specific volume is beneficial to the multiple reflection And scattering of electromagnetic waves,and the PR layer on the surface enhances the stability of the hollow microstructure in the high-temperature pyrolysis process,and is beneficial to the penetration of electromagnetic waves when the hollow microstructure is converted into a derivative carbon layer.Both of them endow the hollow NiCo@C microbox with good microwave absorption properties,and when its thickness is 2.14 mm,the maximum reflection loss peak is-68.4 dB,and the maximum effective absorption bandwidth is 5.8 GHz.Similarly,Wu et al.and Sun et al.Have used biomass carbonization to form hollow mesoporous carbon microspheres as high-performance absorbing materials[66][67]。 In addition,foam structures with high porosity can also be used as high-performance absorbing materials,for example,Zhang et al.Prepared graphene foam by solvothermal method[68]。 Due to the low density,high porosity and good conductivity of the graphene foam,the absorbing properties of the material can be adjusted by simple physical compression,and the total effective absorption bandwidth of the material in different bands is up to 64.5 GHz.Shu et al.Successfully prepared nitrogen-doped reduced graphene oxide/multi-walled carbon nanotube foam composite absorbing material(NRGO/MWCNT)through hydrothermal self-assembly and high temperature calcination,and the detailed preparation process is shown in Fig.2(a)[69]
图2 NRGO/MWCNT复合泡沫材料的 (a) 制备流程图;(b) SEM图;(c) TEM图;(d) 反射损失曲线;(e)吸波机理图[69]

Fig. 2 NRGO/MWCNT composite foam material (a) Preparation process diagram, (b) SEM image, (c) TEM image, (d) Reflection loss diagram, (e) Absorption mechanism diagram [69]

It can be seen from Fig.2(B,C)that the sample is a three-dimensional porous network structure with a pore size between tens of microns and hundreds of microns,and has abundant porosity.in addition,the reduced graphene oxide exhibits rippled and puckered morphologies,and the multi-walled carbon nanotubes are uniformly dispersed on the reduced graphene oxide lamellae.the effects of different preparation conditions on the morphology and microwave absorbing properties of the material were explored by doping Nitrogen into the sample and changing the calcination temperature.the results show that with the increase of calcination temperature,the surface of reduced graphene oxide in the prepared composite foam becomes rougher,and the wrinkled morphology of reduced graphene oxide is more obvious,and the microwave absorption performance of the composite foam is significantly improved with the increase of calcination temperature.In-situ nitrogen doping also significantly enhances the electromagnetic absorption properties of the syntactic foam.As shown in Fig.2(d),the sample is a nitrogen-doped composite foam calcined at 600℃,with a maximum reflection loss peak of-69.6 dB and a maximum effective absorption bandwidth of 4.3 GHz when the thickness is 1.5 mm.Fig.2(e)shows the absorbing mechanism of the material.the good conductive network promotes electron transmission and transition,resulting in dielectric loss.the porous structure is favorable for multiple scattering and reflection of electromagnetic waves to further reduce the electromagnetic waves;nitrogen doping increases the defects and functional groups of the syntactic foam,which is beneficial to the generation of dipole polarization[70]。 Many factors promote NRGO/MWCNT to obtain excellent microwave absorbing properties,so that it has good microwave absorbing ability only by simple nitrogen atom doping and calcination[71]。 In addition,Table 1 lists the synthesis methods,absorption intensity,and absorption bandwidth of different carbon nanomaterials.By comparison,the foam structure,porous structure and nitrogen doping can significantly improve the microwave absorbing properties of carbon nanomaterials。
表1 Comparison of microwave absorbing properties of carbon materials

Table 1 Comparison of the electromagnetic wave absorption performance of carbon materials

Different carbon materials Synthesis method Thickness /mm Reflection loss/dB Absorption bandwidth /GHz Ref.
rGO Chemical reduction 2 6.9 / 58
Graphene foam Solvent heat 10 27 4.2 68
NRGO/MWCNT Hydrothermal method 1.5 69.6 4.3 69
ERG Chemical vapor deposition 3.75 26.7 4.2 72
NCMCCS Solvent heat 3.7 60.4 7.2 73
Metal-free CNTs Chemical vapor deposition 3.5 22.4 1.5 74
CNTs/PyC Template method 6.6 29.6 4.2 75

4 Carbon-based composite radar absorbing material

Carbon nanomaterials have become a strong candidate for electromagnetic wave absorption materials because of their excellent properties[76]。 However,the microwave absorbing properties of single-component carbon nanomaterials can not meet the requirements.Therefore,researchers use them as substrates to prepare composite materials to improve their absorbing properties:(1)carbon materials with different dimensions are compounded to form a special three-dimensional structure to enhance the reflection times of electromagnetic waves in the material,thus improving the absorbing properties of carbon nanomaterials[77~79]; (2)Carbon nanomaterials composite with other materials introduce a new loss mechanism to improve the impedance matching of the composite and enhance its absorbing properties。

4.1 Carbon-carbon composite radar absorbing material

in order to improve the microwave absorbing properties of carbon nanomaterials,two kinds of carbon nanomaterials with different dimensions can be compounded.For example,one-dimensional carbon nanotubes and two-dimensional graphene are compounded to form a three-dimensional structure,so that the defect degree and the specific surface area of the composite material are improved,the dipole polarization is promoted,the dielectric property of the material is enhanced,and the loss of electromagnetic waves in the material is increased.Zhang et al.Grew nitrogen-doped carbon nanotube arrays on ultrathin reduced graphene oxide sheets by freeze-drying and high-temperature carbonization processes using CoNi alloy as a catalyst and melamine as a carbon source,and the experimental process is shown in Fig.3(a)[80]。 As shown in Fig.3(B),the synthesized composite(3D CoNi/N-GCT)has a unique bamboo-like three-dimensional structure,a large specific surface area,and a variety of heterogeneous interfaces,which promote the absorption of electromagnetic waves.in order to verify the effect of the content of carbon nanotubes in the absorbing material on the electromagnetic wave absorption properties,Li et al.Constructed a new type of three-dimensional carbon nanotube network composite absorbing material by phenolic resin template method,and explored the effect of different carbon nanotube content on the absorbing properties[81]。 the composites prepared With different amounts of CNTs and resin were denoted as CNTx/Epoxy,and the conductivity of the samples increased steadily with the increase of CNTs content,as shown in Fig.3(C).the microwave absorbing properties were tested by coaxial method,and the results showed that the microwave absorbing properties first decreased and then increased with the increase of CNTs content,and moved to the low frequency direction with the increase of thickness.When the thickness is 2.9 mm,the CNT5/Epoxy composite has a reflection loss peak of-42.13 dB at 6.4 GHz and an effective absorption bandwidth of 1.6 GHz.with the increase of carbon nanotube content,the electromagnetic wave absorption properties of CNT10/Epoxy composites show a trend to move to the low frequency at the same thickness,but the maximum absorption peak decreases.When the thickness is 3.6 mm,the reflection loss peak is-38.53 dB at 6.2 GHz,and the effective absorption bandwidth is 1.68 GHz,as shown in Fig.3(d,e).This may be due to the high content of carbon nanotubes,which leads to the high surface conductivity of the sample and the skin effect,thus reducing the absorbing properties of the material.On the other hand,the increase of carbon nanotube content leads to the gradual reduction of defects at the edge of the material,which reduces the relaxation polarization of defective carbon atoms。
图3 (a, b) 3D CoNi/N-GCT的合成示意图和TEM图[80];(c) 不同复合材料导电性;(d, e) CNT5/Epoxy和CNT10/Epoxy反射损失曲线[81]

Fig. 3 (a, b) Synthesis schematic and TEM diagram of 3D CoNi/N-GCT [80], (c) Conductivity of different composite materials, (d, e) CNT5/Epoxy and CNT10/Epoxy reflection loss curves [81]

Zhao et al.Prepared carbon nanopolyhedrons(CNPs)-reduced graphene oxide(CNPs/rGO)composites by in-situ pyrolysis using metal-organic framework/graphene oxide hybrids as raw materials[82]。 the electromagnetic parameters of the material can be adjusted according to the amount of GO added.When 32 mL of GO dispersion was added,the microwave absorbing property of the material was the best.When the thickness of the composite is 2.89 mm,the reflection loss peak is-66.2 dB at 6.2 GHz,and the effective absorption bandwidth is 2.2 GHz.Lv et al.Synthesized graphene/carbon nanosphere composite absorbing materials by liquid phase method[83]。 the electrical resistivity of the carbon nanospheres is changed by adjusting the annealing temperature,thereby changing the electromagnetic parameters of the composite.when the annealing temperature is 800℃,the composite has the best absorbing properties,the reflection loss peak is-28.1 dB and the effective absorption bandwidth is 5.7 GHz When the sample thickness is 1.5 mm。
Qiang et al.Prepared carbon microsphere@yolk-like carbon shell composite by"coating-coating etching"method[84]。 The microsphere consists of a core with a diameter of 300 nm,a shell with a thickness of 20 nm,and a gap between the core and the shell.As shown in Fig.4(a,B),the material possesses a large specific surface area of 629 m2·g−1and a high porosity of 0.8 cm3·g−1.The microwave absorbing properties of 50 wt%sample mixed with paraffin were tested,and when the thickness was 2 mm,the reflection loss peak reached-34.8 dB at 15 GHz,and the effective absorption bandwidth was 5.4 GHz.Fig.4(e,f)shows the comparison of the microwave absorption performance between the carbon microsphere and the carbon microsphere@yolk-shaped carbon shell.It can be seen that the addition of the yolk-shaped carbon shell structure significantly enhances the electromagnetic wave absorption performance.This is due to the fact that the impedance of the hollow carbon shell matches the impedance of free space,and the electromagnetic wave is easier to enter the interior of the material,and multiple scattering and reflection between the core and shell lead to increased electromagnetic wave loss.On the other hand,as shown in Fig.4(C,d),the relative complex permittivity of carbon microsphere is much higher than that of carbon microsphere@yolk-like carbon shell,while the complex permeability of the two materials is almost equal.However,the large difference between complex permittivity and complex permeability is not conducive to the impedance matching of the material,which leads to strong reflection of electromagnetic waves on the surface of the absorbing material.Therefore,the microwave absorbing properties of carbon microspheres are poor 。
图4 碳微球和碳微球@蛋黄状碳壳的 (a) N2吸附曲线;(b) 孔径分布;(c) 相对复介电常数;(d) 相对复磁导率;(e, f) 反射损失3D图[84]

Fig. 4 (a) N2 adsorption-desorption isotherm, (b) Pore size distribution, (c) Complex permittivity, (d) Complex permeability, (e, f) Reflection loss 3D diagram of C microspheres and yolk-shell C@C microspheres[84]

to sum up,carbon-carbon composite radar absorbing material is a composite radar absorbing material with large specific surface area,high porosity and hollow structure,which is composed of two carbon materials with different dimensions by in-situ growth,high temperature carbonization and hydrothermal method.Uch as bamboo-shaped three-dimensional carbon nanotube arrays,yolk-shell-shaped carbon microspheres and the like.as a double dielectric system,the conduction loss becomes the main reason for the dissipation of electromagnetic energy,and the dipole polarization and interface polarization provide auxiliary contributions to the consumption of electromagnetic energy.electromagnetic waves are consumed by compounding two carbon materials to form a porous structure,introducing defects,and constructing a three-dimensional conductive network.the porous three-dimensional structure makes the electromagnetic wave reflected and scattered many times in the material,which leads to the enhancement of electromagnetic wave loss.Secondly,the abundant defects and functional groups On the surface produce more dipole polarization and interfacial polarization.on the other hand,the unique three-dimensional conductive network promotes the conductive loss of electromagnetic waves.However,despite the excellent characteristics of carbon-carbon composites,carbon materials still face problems such as high dielectric constant,poor impedance matching,and narrow effective bandwidth of absorption.Compositing carbon materials with magnetic materials is an effective way to solve the above problems[85]

4.2 Carbon-metal/metal oxide composite radar absorbing material

magnetic materials with low coercivity and high saturation magnetization can produce characteristic Magnetic interaction with electromagnetic waves,resulting in excellent attenuation of electromagnetic waves[86]。 magnetic materials such as iron,cobalt,nickel and their oxides are compounded with carbon nanomaterials,which can effectively introduce Magnetic loss and improve the permeability of carbon materials,thus improving the absorbing properties of composite materials。
Hou et al.Prepared MWCNTs/Fe3O4composite by hydrothermal method,and studied the effect of Fe2+and Fe3+concentration of the composite in X-band on its microwave absorbing properties[87]。 When the concentrations of Fe2+and Fe3+are 0.02 and 0.04 mol·L−1,respectively,the MWCNT/Fe3O4composite shows better absorbing properties with a reflection loss peak of−18.22 dB at 12.05 GHz.Zhu et al.Used a hydrothermal method to embed Fe3O4submicrospheres into rGO to form Fe3O4/rGO composites,and the dielectric properties of the composites were regulated by changing the amount of rGO addition[88]。 When the addition of rGO is 4 wt%,the balance between permittivity and permeability of the material reaches the best level,and the impedance matching is improved.When the thickness is 3.5 mm,the reflection loss peak of the material reaches−45 dB,and the effective absorption bandwidth is 3.2 GHz.Wu et al.Prepared a novel amorphous iron/graphene oxide nanocomposite by one-step chemical reduction method,and the preparation process is shown in Fig.5(a)[89]。 When Fe2+ions and GO are simultaneously reduced to amorphous Fe and rGO during the reduction process,the rGO flakes can provide abundant nucleation conditions and growth sites for Fe,resulting in heterogeneous nucleation of Fe nanoparticles on the rGO surface.The formed amorphous iron particles were uniformly dispersed and firmly embedded into the reduced graphene oxide surface,as shown in Fig.5(B).When the addition of graphene oxide is 5 wt%,the composite has excellent microwave absorption properties,as shown in Fig.5(C).When the thickness is 3.26 mm,the reflection loss peak is as high as−72.8 dB at 7.28 GHz,and the effective absorption bandwidth is 5.9 GHz.Because reduced graphene oxide is a non-magnetic material,the saturation magnetization and coercivity of the composite decrease with the increase of reduced graphene oxide content.The reduction of coercivity is beneficial to the improvement of absorbing performance,and its hysteresis loop is shown in Fig.5(d).The excellent microwave absorbing properties of the composite are due to its low coercivity and high saturation magnetization,which maximize the magnetic loss.Secondly,the combination of reduced graphene oxide with excellent dielectric properties makes the magnetic loss and dielectric loss in the composite material play a synergistic role,so that the material has excellent impedance matching and electromagnetic wave attenuation ability.Lv et al.Prepared layered hollow carbon nanospheres@Fe@Fe3O4composites by template method and thermal cracking method,and the microwave absorbing properties of the composites could be controlled by adjusting the thickness of the hollow carbon nanospheres[90]。 the material has excellent microwave absorbing properties due to the interfacial polarization generated by a variety of heterogeneous interfaces.When the thickness is 1.5 mm,the reflection loss peak is−40 dB,and the effective absorption bandwidth is 5.2 GHz.Kim et al.Designed a new electroless plating method without heat treatment to prepare FeCoNi@graphene composite absorbing film[91]。 Due to the good impedance matching of the composite,the peak reflection loss is as high as−68 dB at 8.4 GHz when the thickness is 2.33 mm.Ding et al.Mixed Co3O4nanosheets prepared by hydrothermal method with rGO to obtain Co3O4/rGO composite[92]。 Due to the excellent dielectric properties and polarization ability of rGO and the excellent magnetic loss of the Co3O4sheet,the material exhibits a reflection loss peak of−45.15 dB and an effective absorption bandwidth of up to 7.14 GHz at a thickness of 3.6 mm.Chen et al.Used a solvothermal method to load Fe3O4on sulfur-doped graphene,which provided a good condition for material dipole polarization because the surface of the material was rich in polar bonds C-S[93]。 In addition,due to the improvement of impedance matching ability and the introduction of magnetic loss,the composite has excellent microwave absorbing properties.At a thickness of 2 mm,the reflection loss peak is−41 dB,and the effective absorption bandwidth is 5.3 GHz。
图5 非晶Fe/rGO复合材料的 (a) 制备流程示意图;(b) TEM图;(c) 反射损失曲线;(d) 磁滞回线图[89]

Fig. 5 (a) Preparation process diagram, (b) TEM images, (c) Reflection loss curve, (d) Hysteresis diagram of amorphous Fe/rGO composites [89]

metal-organic frameworks(MOFs)are a class of crystalline porous materials composed of Metal nodes joined together by organic ligands through strong coordination bonds,and they are also considered to be excellent precursors for various carbon-based functional materials due to the pyrolysis of organic ligands at high temperature in an inert atmosphere[94~96]。 MOF has many excellent features that make it an excellent precursor for high-performance microwave absorbers.Qiang et al.Took the lead in synthesizing uniform Fe/C composites by direct pyrolysis of organic framework Prussian blue nanocubes,and found that the high dispersion of Fe nanoparticles is conducive to multiple dielectric and magnetic resonance,resulting in excellent electromagnetic absorption properties and wide response bandwidth,with a maximum effective absorption bandwidth of 7.2 GHz[97]。 Yin et al.prepared dodecahedral porous carbon nanotube/cobalt nanoparticle composite(CNTs/Co)by in-situ pyrolysis method using cobalt-based zeolite imidazole ester framework(ZIF-67)as precursor,and explored The effect of pyrolysis temperature on the morphology and microstructure of the composite.the preparation process is shown in Fig.6(a)[98]。 as shown in Fig.6(B),the surface of the dodecahedron is distributed with high density of short and curved carbon nanotubes.when the pyrolysis temperature increases to 900℃,the amount of Co nanoparticles attached increases and the dispersion is good.with the further increase of pyrolysis temperature,although the growth of carbon nanotubes and the graphitization degree of the material can be promoted,the Co nanoparticles will reaggregate and seriously damage the magnetic loss.Therefore,when the pyrolysis temperature is 900℃,the microwave absorbing property of the composite is the best.As shown in Fig.6(C,d),when the thickness is 1.81 mm,the reflection loss peak at 15 GHz is−60.4 dB,the effective absorption bandwidth is 5.2 GHz,and the position of the absorption peak is consistent with the quarter-wavelength cancellation law.Fig.6(d)is a schematic diagram of the absorbing mechanism of the CNTs/Co composite,and the reasons for its excellent absorbing performance are As follows:(1)due to the multi-plane and large specific surface area of the material,electromagnetic waves are scattered and reflected multiple times inside the material[99]; (2)that surface of the carbon nanotube contain a large number of defect and oxygen-containing functional groups to promote dipole polarization;(3)interfacial polarization between Co particles and carbon nanotubes;(4)that carbon nanotube are mutually contacted to form a conductive network to generate resistance type Los;(5)that transition of electron between different interfaces further consume electromagnetic wave energy;(6)Co particles produce excellent magnetic losses。
图6 CNTs/Co复合物的 (a) 制备流程示意图;(b) TEM图;(c, d) 900 ℃下的反射损失及匹配厚度曲线图;(e) 电磁波吸收机理[98]

Fig. 6 (a) Schematic diagram of preparation process, (b) TEM images, (c, d) Reflection losses and dependence of matching thicknesses at 900 ℃, (e) Electromagnetic wave absorption mechanism of CNTs/Co Composite[98]

ferrite absorbing material is a kind of material based on the principle of absorbing electromagnetic wave by magnetic loss.Compared with other radar absorbing materials,it has the advantages of high frequency,wide frequency band and thin coating.Commonly used ferrite soft magnetic materials are manganese-zinc,nickel-copper-zinc,magnesium-copper-zinc,nickel-magnesium-zinc and ultra-high frequency soft magnetic ferrite of planar hexagonal system[100~102]。 However,its high density and poor oxidation resistance have seriously hindered the wide application of the material.To overcome these problems,composites with carbon materials are commonly performed。
Zhang et al.Used solvothermal method to attach CoFe2O4nanoparticles on carbon nanotubes to synthesize CoFe2O4/CNTs composite[103]。 Cobalt ferrite nanoparticles not only have the characteristics of traditional microwave absorbing materials,but also have high permeability at high frequency,which can improve the microwave absorbing properties to a certain extent by combining with CNTs to form composites.Wang et al.Synthesized a CoFe2O4/nitrogen-doped redox graphene aerogel(CNGA)composite with a three-dimensional porous structure by solvothermal method and freeze-drying,the synthesis process is shown in Fig.7(a),and explored the effect of different CoFe2O4additions on the absorbing properties of the composite[104]。 The addition of CoFe2O4in the three samples showed an increasing relationship,which was marked as CNGA-1,CNGA-2,CNGA-3.Interestingly,as shown in Fig.7(B),the C0of the three samples do not change in the frequency range of 5~18 GHz,which proves that the eddy current loss is the main magnetic loss in this frequency band[106]。 With the increase of CoFe2O4content,the attenuation ability of the material to electromagnetic wave is weakened,which is attributed to the re-agglomeration of magnetic CoFe2O4particles and the decrease of magnetic loss ability of the material.In addition,due to the appropriate ratio of CoFe2O4and rGO,CNGA-2 among the three samples shows excellent impedance matching,and its absorbing properties are shown in Fig.7(C,d).When the sample filling amount is 20 wt%and the thickness is 2.1 mm,the reflection loss peak is as high as−60.4 dB,and the effective absorption bandwidth is 6.48 GHz.At the same time,when its thickness is 3 mm,it can fully absorb the X-band.The absorbing mechanism of the composite is shown in Fig.7(e).The three-dimensional porous structure causes multiple reflection and scattering of electromagnetic waves,which is beneficial to the attenuation of electromagnetic waves.Aerogel with high specific surface area produces rich dipole polarization,interface polarization and defect polarization,thus increasing the polarization loss of the material;At the same time,the three-dimensional conductive network promotes electron transmission and transition,and improves the resistance loss of the material;In addition,the eddy current loss generated by the CoFe2O4nanoparticles enhances the magnetic loss of the material.Zong et al.Synthesized rGO/CoFe2O4composites by hydrothermal method,and proved that different reduction degrees of graphene oxide would change the electromagnetic parameters of the composites,thus obtaining different microwave absorbing properties[107]。 Graphene oxide was reduced by two different reducing agents to obtain rGO composites with different degrees of reduction.By changing the C/O ratio and the number of oxygen-containing functional groups on the surface of the material,the electromagnetic parameters of the composite are changed,thus changing its absorbing properties.He et al.Used the same method to prepare NiFe2O4/rGO composites by uniformly depositing magnetic nickel ferrite nanoparticles on reduced graphene oxide nanosheets,and explored the effects of NiFe2O4in the composites[108]。 The NiFe2O4induces a variety of polarization relaxation and natural resonance phenomena,which change the permeability and permittivity of the composite,thus improving the absorbing properties of the material.When the thickness is 5 mm,the reflection loss peak of the material is-42 dB,and the effective absorption bandwidth is 5.3 GHz.Shu et al.Prepared multiwalled carbon nanotube/zinc ferrite composite(MWCNTs/ZnFe2O4)by solvothermal method[109]。 The ZnFe2O4microsphere is fixed on the surface of the MWCNTs,and the ZnFe2O4microsphere has high saturation magnetization and low coercive force,so that the magnetic loss is introduced,and the dielectric loss of the composite material is increased.When the sample thickness is 1.5 mm,the reflection loss peak reaches−55.5 dB at 13.4 GHz,and the effective absorption bandwidth is 3.6 GHz.Wang et al.Combined spray drying,solvothermal and calcination to prepare a flower-like CoFe2O4@graphene composite with gossamer-like graphene wrapping CoFe2O4microspheres[110]。 This unique structure can effectively reduce the stacking of graphene,thereby improving the electromagnetic wave absorption performance of the composite.When the thickness is 2 mm,the reflection loss peak is-42 dB at 12.9 GHz,and the effective absorption bandwidth is 4.59 GHz.Lin et al.Prepared three-dimensional porous Bi2Fe4O9microspheres/reduced graphene oxide(Bi2Fe4O9/rGO)composite using a one-step etching method with flaky Bi2Fe4O9as the precursor[111]。 As shown in Fig.8(a~C),the Bi2Fe4O9microspheres with an average diameter of 500 nm were uniformly grown on the graphene sheet.In addition,it can be seen from Fig.8(C)that after etching,a large number of pores appear on the surface of the Bi2Fe4O9,the specific surface area of the composite is significantly increased,and the electromagnetic wave can produce more scattering and reflection,thus enhancing the absorbing performance of the composite.The porous Bi2Fe4O9microspheres improve the dielectric loss and magnetic loss of the composite,as shown in Fig.8(d),when the sample thickness is 2 mm,the reflection loss peak is as high as−71.88 dB at 13.8 GHz,the effective absorption bandwidth is 4.24 GHz,and the absorption peak position follows the quarter-wave cancellation law.Fig.8(e)is a schematic diagram of the absorbing mechanism of the composite.Because that composite material has high-conductivity graphene and high-porosity Bi2Fe4O9microsphere,electromagnetic waves are subject to multiple scattering and reflection in the composite material;The porous structure of Bi2Fe4O9and the functional groups in rGO will break the charge distribution balance and cause dipole polarization and relaxation process.The interface polarization between two phases plays an important role in the absorption of electromagnetic waves 。
图7 CFO/N-rGO气凝胶(CNGA)的 (a) 合成路线图;(b) C0-f曲线;(c) 吸波性能对比图;(d) CNGA-2反射损耗图;(e) 吸波机理示意图[104,105]

Fig. 7 (a) Schematic illustration of the synthetic route, (b) the C0-f curves, (c) Absorption performance comparison, (d) Reflection loss diagram of CNGA-2, (e) Schematic illustration on wave absorption mechanism of CFO/N-rGO aerogel (CNGA)[104,105]

图8 Bi2Fe4O9/rGO复合材料的 (a~c) SEM图;(d) 反射损失图;(e) 吸波机理示意图[111]

Fig. 8 (a~c) SEM image, (d) Reflection loss diagram, (e) Schematic illustration on wave absorption mechanism of Bi2Fe4O9/rGO composite material[111]

Similarly,Gao et al.Prepared three-dimensional porous BiFeO3microspheres/reduced graphene oxide(BiFeO3/rGO)composite by the same method using BiFeO3particles and graphene oxide as precursors[112]。 The specific process is as follows:the precursor and the graphene oxide are subjected to dissolution,crystallization,re-reduction and the like to generate a large number of small lamellar BiFeO3and reduced graphene oxide,and finally the three-dimensional porous structure composite radar absorbing material is formed through self-assembly.When the thickness of the composite is 1.8 mm,the peak reflection loss is-46.7 dB,and the effective absorption bandwidth is 4.7 GHz.Zhao et al.Prepared carbon nanotube-linked expanded graphite sandwich composite(CNT/EG/BF)with BaFe12O19metal particles in the middle by sol-gel method[113]。 CNTs make the BaFe12O19metal particles and expanded graphite interconnected and form a special three-dimensional conductive network,which increases the conductivity and dielectric loss of the composite,and the sandwich structure is conducive to the multiple scattering and reflection of electromagnetic waves.When the thickness of the sample is 1 mm,the peak reflection loss is-45.8 dB at 14.2 GHz,and the effective absorption bandwidth is 2.3 GHz 。
In addition to the design of carbon nanomaterials/ferrite composite structure to improve its absorbing properties,the ferrite can also be doped to improve the dielectric loss and magnetic loss of the ferrite.For example,Bibi et al.Synthesized copper-doped ferrite/multi-walled carbon nanotube(Cu0.25Ni0.25Zn0.5Fe2O4/MWCNTs)composite by co-precipitation method[114]。 Copper doping improves the saturation magnetization and conductivity of ferrite,and forms a good conductive network with MWCNTs.When the sample thickness is 2.5 mm,the reflection loss peak is-37.7 dB at 10.2 GHz,and the effective absorption bandwidth is 4.1 GHz.Liu et al.Prepared a novel cobalt-doped nickel-zinc ferrite/graphene composite(Co0.2Ni0.4Zn0.4Fe2O4/GN)B y hydrothermal method[115]。 The Co0.2Ni0.4Zn0.4Fe2O4nanoparticles were uniformly covered by graphene,thus preventing the agglomeration of magnetic particles.In addition,with the increase of the graphene content,the conductivity of the composite material is improved,and the dielectric loss capability of the composite material for electromagnetic waves is further enhanced.When the sample thickness is 5.5 mm,two absorption peaks appear at 9.6 GHz and 5.2 GHz,and the corresponding reflection loss peaks are-53.5 dB and-58.3 dB,respectively,and the effective absorption bandwidth is up to 14.8 GHz.Shu et al.Synthesized nitrogen-doped reduced graphene oxide/nickel-zinc ferrite(N-rGO/Ni0.5Zn0.5Fe2O4)composite by a two-step method using graphene oxide as a template[116]。 When the sample thickness is 2.91 mm,the reflection loss peak is-63.2 dB,and the effective absorption bandwidth is 5.4 GHz。
Recently,carbon nanohorns have aroused great interest of many scholars,and our research group has been studying in the field of carbon nanohorns for many years,and has verified their excellent microwave absorbing properties.Single-wall carbon nanohorns(SWCNHs)are closed hollow pyramidal structures composed of carbon atoms bonded by wall carbon nanohorns,with a diameter of 2~5 nm and a length of 40~50 nm.They cannot exist alone under normal conditions,and most of them exist in the form of spherical aggregates aggregated by thousands of SWCNHs[117]。 Because of its low density,large specific surface area,excellent electrical and thermal conductivity,it has been widely used in electrochemistry,sensors,metal batteries,medical treatment and catalysts[118,119]。 At the same time,compared with other carbon materials,SWCNHs have the following advantages:(1)the preparation process does not need a metal catalyst and has higher purity[120]; (2)It is highly modifiable and can provide more surface active sites[121]; (3)the spherical aggregate structure with a diameter of 50~100 nm makes SWCNHs have a high specific surface area;(4)the SWCNHs aggregate has a large internal space,allowing the encapsulated molecules to move freely.in addition,SWCNHs also have Many advantages in electromagnetic wave absorption:the urchin-like spherical aggregate of SWCNHs is beneficial to multiple scattering and reflection of electromagnetic waves,and the unique conical structure is beneficial to impedance matching of the material;More surface active sites are beneficial to the composite of other materials.many advantages make SWCNHs have great potential in the field of microwave absorption.For example,Zhang et al.Synthesized N-doped carbon nanohorns coated with Co particles(Co@N-CNHs)by DC arc plasma[122]。 in the process of arc plasma discharge,the content of metal Co in the composite material can be changed by evaporating the carbon rod anode with Co wires inserted in the middle and adjusting the number of Co wires in the carbon rod.Due to the unique conical structure of carbon nanohorns and magnetic cobalt particles,the composite material has excellent impedance matching,and electromagnetic waves can better enter the material,so that its wave absorption capacity can be improved.When the sample thickness is 2.5 mm,the reflection loss peak is-41.39 dB at 7.3 GHz.Zhang et al.Prepared N-doped carbon nanohorn coated Fe nanoparticle composite(Fe@N-CNHs)by the same method,and changed the loading of Fe in carbon nanohorns by adjusting the number of Fe wires,and the preparation process is shown in Fig.9(a)[123]。 the"dahlia-like"carbon nanohorn aggregates prepared by direct arc current plasma uniformly wrap the Fe nanoparticles,showing excellent microwave absorbing properties,as shown in Fig.9(B,C).When the sample thickness is 1.6 mm,the maximum reflection loss peak is−44.52 dB at 10.86 GHz,and the maximum effective absorption bandwidth is 3.23 GHz.Fig.9(d)shows the absorbing mechanism of the material.the unique conical structure of the carbon nanohorn makes it have a large specific surface area,which is conducive to multiple scattering and reflection of electromagnetic waves and enhances the attenuation of electromagnetic waves.Secondly,the dielectric loss of the composite is enhanced due to the dipole polarization produced by the doping of N atoms in the CNHs lattice.in addition,the interfacial polarization can be effectively controlled by adjusting the content of Fe nanoparticles encapsulated in CNHs,and the magnetic loss is enhanced by the introduction of magnetic particles。
图9 Fe@NCNHs复合材料的 (a) 制备示意图;(b) 反射损失峰值图;(c) RL值3D投影图;(d) 吸波机理示意图[122]

Fig. 9 Fe@NCNHs composite materials of (a) Preparation diagram, (b) Reflection loss diagram, (c) 3D projection of RL values, (d) Schematic diagram of absorbing mechanism[122]

In a word,carbon-metal/metal oxide composite absorbing materials have become the focus of absorbing research because of their excellent absorbing properties and multi-loss mechanism.the carbon-metal/metal oxide composite absorbing material is finally formed by coating a carbon layer on the surface of the metal/metal oxide by a solvothermal method,a sol-gel method,a hydrothermal method and the like,or loading a ferrite on a carbon material by electrostatic adsorption,physical mixing and other means.carbon coating with high chemical stability is beneficial to improve the oxidation resistance and corrosion resistance of metal materials,and improve the service life of composite materials.Secondly,the carbon material loaded with magnetic metal can effectively prevent the agglomeration of magnetic metal and give full play to the magnetic loss of magnetic metal,and the addition of carbon material effectively reduces the overall quality of the composite material,which meets the lightweight requirements of absorbing materials。
with the introduction of magnetic metals,carbon-based composite absorbing materials will produce a variety of loss mechanisms,such as dielectric loss,conductive loss and magnetic loss.the good magnetic properties of magnetic metals contribute to excellent magnetic losses,which promote the dissipation of electromagnetic waves through a variety of interactions with electromagnetic fields,such as natural resonance,exchange resonance,and eddy current loss;On the other hand,by controlling the morphology and doping other metals to change the composition and structure of the ferrite,such as flaky magnetic metal,flower-like aggregate,copper ferrite,zinc ferrite and the like,the saturation magnetization and permeability of the magnetic metal can be effectively improved,so that the composite absorbing material with excellent electromagnetic wave absorption performance can be obtained。

4.3 Carbon-ceramic composite radar absorbing material

high temperature environment is one of the important application scenarios of radar absorbing materials,and ceramic materials have good high temperature resistance.Compositing ceramics with carbon materials can not only obtain composite materials with high temperature resistance,wear resistance and corrosion resistance,but also combine dielectric loss with resistive loss to improve the absorbing properties of composite materials。
Han et al.Prepared a graphene/silicon carbide nanowire ceramic composite by polymer pyrolysis process[124]。 Graphene promotes the heterogeneous nucleation of silicon carbide nanowires at low temperatures,and the two form a layered structure through self-assembly.When the thickness of the sample is 2.35 mm and the addition of graphene is 3 wt%,the peak reflection loss is-69.3 dB at 10.55 GHz.In addition,the resistivity and dielectric constant of the material increase with the increase of temperature,and the absorbing properties of the material are improved.When the temperature is 673 K and the thickness of the sample is 2.3 mm,the composite shows the best absorbing properties,and the maximum reflection loss peak is-50.13 dB at 11.67 GHz.Wen et al.Prepared MWCNTs/SiO2composite powders by mixing 2 wt%,5 wt%,10 wt%MWCNTs with silica,grinding and sintering using ultrasonic method[125]。 When the content of MWCNTs is 5 wt%and the thickness of the sample is 3.5 mm,the maximum reflection loss peak of the composite powder is-60.54 dB at 573 K,and the effective absorption bandwidth is 4.2 GHz.Cao et al.Mixed rGO with SiO2powder and prepared the composite by cold briquetting[126]。 Combining the rGO conductivity and SiO2dielectric properties,the composite radar absorber with 2.1 mm thickness was obtained,and the reflection loss peak-42 dB at 413 K temperature and the effective absorption bandwidth of 4.2 GHz were obtained.Lu et al.Used the solution method to adsorb ZnO nanocrystals on the surface of multi-walled carbon nanotubes and added SiO2to form the composite[127]。 At the same time,the high temperature dielectric properties and electromagnetic wave absorption properties of the material in the range of 373~673 K were studied.The addition of the ZnO crystal improves the dielectric property of the carbon material,and the SiO2improves the thermal stability of the composite material,so that the material still has excellent microwave absorbing property at high temperature.Wang et al.Used phosphomolybdic acid/polypyrrole(PMo12/PPy)nanospheres simply polymerized at room temperature as a precursor to successfully construct pomegranate-shaped Mo2C@C nanospheres by high temperature pyrolysis under inert atmosphere,and the tiny Mo2C nanoparticles were coated with ultrathin carbon shells and uniformly dispersed in the carbon matrix[128]。 Both of them are dielectric materials,and the conduction loss is the main reason for the electromagnetic energy dissipation of Mo2C@C nanospheres,and the dipole polarization and interface polarization provide auxiliary contributions in this process.Lian et al.Successfully prepared tungsten carbide/carbon composites by using a solid mixture of dicyandiamide(DCA)and ammonium metatungstate(AM)as precursors,in which ultrafine cubic tungsten carbide nanoparticles were grown in situ and uniformly dispersed on carbon nanosheets during high temperature pyrolysis[129]。 When the ratio of DCA to AM is 6:1,the two samples show good microwave absorption properties,the strongest reflection peak value is-55.6 dB,and the qualified absorption bandwidth covers the frequency range of 3.6~18.0 GHz。
To sum up,carbon-ceramic composite radar absorbing materials have excellent radar absorbing properties at high temperature.carbon materials and resistive materials,such as silicon carbide nanowires and silicon dioxide powder,were compounded by high temperature pyrolysis,ultrasonic mixing,mechanical cold pressing and other methods,and finally carbon-ceramic composite absorbing materials were prepared.On the one hand,the conductive loss and dielectric loss capabilities of the composite absorbing material are enhanced,and the absorbing properties of the composite material can be regulated and controlled by adjusting the content of the ceramic powder;On the other hand,ceramic materials have the characteristics of strong thermal stability,high hardness,corrosion resistance,wear resistance and high temperature resistance,which greatly enhance the application of carbon-ceramic composite absorbing materials in extreme environments and prolong the service life of materials.Although carbon-ceramic composite radar absorbing materials have many excellent characteristics,the weight of ceramic materials can not be ignored,which also affects the requirement of lightweight radar absorbing materials and seriously limits their practical application。
Finally,different types of carbon-based composite absorbing materials formed by structure design,composition design,introduction of magnetic metal and ceramic powder show excellent absorbing properties.As shown in Table 2,the synthesis methods,reflection loss peak,and effective absorption bandwidth of some carbon-based composite absorbing materials are listed。
表2 Comparison of electromagnetic wave absorption properties of different carbon matrix composites

Table 2 Comparison of electromagnetic wave absorption performance of various carbon-based composited materials

Carbon-based composite absorbing materials Synthesis method Thickness /mm Reflection loss/dB Absorption bandwidth /GHz Ref.
CNT5/Epoxy Hydrothermal method 2.9 42.13 1.6 81
CNPs/rGO In-situ pyrolysis 2.89 66.2 14.8 82
GN/CS Liquid-phase method 1.5 28.1 5.7 83
Yolk-shell C@C Co-precipitation, Etching 2 34.8 5.4 84
MWCNTs/Fe3O4 Hydrothermal method / 18.22 / 87
Fe3O4/rGO Hydrothermal method 3.5 45 3.2 88
Amorphous Fe/RGO Solvent heat 3.26 72.8 5.9 89
C@Fe@Fe3O4 Template method, Pyrolysis 1.5 40 5.2 90
FeCoNi@GO Chemical plating 2.33 68 8.4 91
Co3O4/rGO Hydrothermal method 3.6 45.15 7.14 92
Fe3O4/S-GO Solvent heat 2 41 5.3 93
CNTs/Co In-situ pyrolysis 1.81 60.4 5.2 98
CoFe2O4/CNTs Solvent heat / 15.7 2.5 103
CoFe2O4/N-rGO Solvent heat 2.2 60.4 6.48 104
rGO/CoFe2O4 Hydrothermal method 2.3 47.9 5 107
MWCNTs/ZnFe2O4 Hydrothermal method 1.5 55.5 3.6 109
CoFe2O4@GO Solvent heat 2 42 12.9 110
Bi2Fe4O9/rGO One-step etching 2 71.88 13.8 111
BiFeO3/rGO One-step etching 1.8 46.7 4.7 112
CNT/EG/BF Sol-gel method 2 26.1 8.2 113
Cu0.25Ni0.25Zn0.5Fe2O4/
MWCNTs
Co-precipitation 2.5 37.7 / 114
Co0.2Ni0.4Zn0.4Fe2O4/GN Hydrothermal method / 58.3 14.8 115
N-rGO/Ni0.5Zn0.5Fe2O4 Solvent heat 2.91 63.2 5.4 116
G/SiOC Polymer pyrolysis 2.35 69.3 3.9 124
MWCNTs/SiO2 Ultrasonic method 3.5 60.54 4.2 125
rGO/SiO2 Cold pressing method 2.1 42 4.2 126
Mo2C@C Pyrolysis 1.9 48 4.1 128

5 Conclusion and prospect

in this paper,the absorption mechanism of electromagnetic wave is summarized from the aspects of impedance matching,loss mechanism and attenuation constant,and the research progress of preparation process,morphology characteristics and absorbing properties of various carbon nanocomposite absorbing materials is discussed.Compared with traditional radar absorbing materials,carbon materials have unique advantages such as high conductivity,light weight,good chemical stability and excellent mechanical properties.Although single carbon materials show great potential,limited attenuation mechanisms and poor impedance matching greatly hinder their practical applications.Compositing carbon materials with other materials is an effective way to break through the above bottleneck.For carbon-based composite absorbing materials,the construction of a unique three-dimensional structure with high specific surface area,porosity and heterogeneous interface is conducive to the multiple reflection and scattering of electromagnetic waves,thereby enhancing the dielectric loss and multiple polarization relaxation of the material.On the other hand,by introducing a magnetic metal,its excellent magnetic loss contributes to various interactions between the composite and the electromagnetic field,such as natural resonance,exchange resonance,and eddy current loss.At the same time,the synergistic effect between the magnetic loss and the dielectric loss helps to improve the impedance matching of the composite material,thereby enhancing the attenuation capability of electromagnetic waves;In addition,by compounding with ceramic powder with high thermal stability,it is beneficial to improve the service life of carbon-based composite absorbing materials In high temperature environment。
in recent years,with the emergence of more and more extreme application scenarios,higher requirements for absorbing materials have been put forward.carbon nanomaterials exhibit excellent oxidation and corrosion resistance in extreme environments due to their excellent chemical stability,which is beneficial to enhance the service life of carbon-based composite absorbing materials in extreme environments.Despite the substantial progress made so far in carbon-based composite absorbing materials,there are still many problems and challenges。
(1)Due to the influence of raw materials,preparation process and other factors,there are great differences in the purity,structural defects,porosity and specific surface area of the prepared carbon nanomaterials,which leads to the instability of the absorbing properties of carbon nanomaterials and seriously affects their absorbing properties.At the same time,the preparation process of composite materials is complex and requires high temperature and high pressure conditions,which is not easy for large-scale production.Therefore,the exploration of carbon-based composite absorbing materials with simple preparation process and green environmental protection is the direction of future efforts。
(2)In addition to performance characterization,the practical application of absorbing materials should also be considered to meet the requirements of"thin,wide,light and strong",and the development of multifunctional absorbing materials with high temperature resistance,oxidation resistance,acid and alkali resistance and corrosion resistance will be the development trend。
(3)the absorbing mechanism of carbon matrix composites should be further analyzed,but most of the research stays on the design of structure and components,and there is a lack of in-depth research on the absorbing mechanism.Therefore,it is very important to study the absorption mechanism of carbon-based composite absorbing materials。
(4)In addition to the structural design and composition design of absorbing materials,heterogeneous interface engineering,atom doping engineering and defect engineering need to be developed.the introduction of multiple heterointerfaces,lattice defects,magnetic heteroatoms and microporous structures can change the energy band arrangement,electron transmission,space charge distribution and electromagnetic wave propagation path of the composite,which will greatly enhance the absorbing performance of the composite absorbing material。
Finally,based on the unique advantages of carbon-based composite absorbing materials,combined with its fine structural design and excellent absorbing properties,microwave absorbing devices can be miniaturized and lightweight,which lays the foundation for the practical application of absorbing materials.At the same time,it also brings unlimited potential for the integration of carbon-based composite absorbing materials and intelligent devices to develop in the direction of diversification,intelligence and multi-function.We firmly believe that carbon-based composite radar absorbing materials have extremely bright prospects and great practical potential in aerospace,military,electronic information,intelligent equipment,new energy and other fields。
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