基于VO2、NaF和TiO2材料的红外线超宽带吸收器

Infrared Ultra-Wide-Band Absorber Based on VO_(2),NaF,and TiO_(2)

设计了一种基于VO_(2)、NaF和TiO_(2)材料的红外线超宽带可调吸收器,并采用有限元方法对其吸收特性进行了分析。结果表明:当入射波垂直入射时,吸收率对偏振角不敏感。在21~25μm及35~43μm波长范围内,吸收率可以达到99.8%。在12~51μm范围内,吸收率可以达到90%。在0~55°入射角范围内,横磁(TM)波在12~52μm波长范围内,横电(TE)波在20~45μm波长范围内,吸收率均可达到80%以上。获得宽带吸收的主要原因是表面等离子体共振效应。通过改变VO_(2)的电导率,可以调节吸收器的吸收率,实现吸收率的可调性。所设计的红外线超宽带吸收器具有优良的吸收性能,在传感、探测及能量收集和转化等方面具有潜在的应用价值。

Objective Electromagnetic wave absorbers operating in the microwave,THz,infrared,visible,and ultraviolet bands have become a prevalent research topic.The typical electromagnetic wave absorber is a vertically stacked multilayer structure based on a metal-dielectric-metal(MIM)structure.The optical characteristics of metal,semiconductor,and new materials can be utilized to optimize the absorption of incoming electromagnetic waves.Absorption mechanisms such as local plasmon resonance,magnetic polariton resonance,surface plasma resonance,Fabry-Perot cavity resonance,and guide mode resonance can be used to realize ideal absorption effects.Infrared absorbers with efficient,broadband,and tunable properties are urgently required in optical sensors,photothermal energy converters,imaging,and infrared stealth cloaks.However,in practical applications,achieving a broadband response in the infrared band is difficult.Most proposed infrared absorbers are limited to the near-infrared(NIR)range and are untunable.Therefore,an ultra-broadband tunable absorber operating from near-infrared to far-infrared is proposed,and its absorption mechanism is analyzed.Methods An infrared broadband absorber is designed based on the phase material VO_(2),metalloids,and high-temperature resistance materials NaF and TiO_(2).First,owing to the unique properties of the materials,the material properties are set based on the role and characteristics of different materials.The ports at the upper and lower ends along the z-direction are set separately,the port type is periodic,and the two ports are set to open and close,respectively.Second,the domains,boundaries,and edges of the different materials in the structure are meshed in detail.Parametric sweeping is then performed according to the study band,and the electric field distribution and the magnetic field are obtained.Finally,the optimal result is obtained through repeated calculations by adjusting the structural geometric parameters,angle of incidence,and polarization angles of the transverse electric(TE)and transverse magnetic(TM)waves.Results and Discussions After several simulations,the optimization parameters are obtained:the cell period is 7μm,the width of the bottom composite layer is 5.8μm,the width of the top composite layer is 3.4μm,the thickness of Au is 0.9μm,the thickness of SiO_(2) layer is 0.9μm,the thickness of NaF layer is 0.1μm,the thickness of VO_(2) layer is 1.0μm(the conductivity is set as 2×1015 S/m),and the thickness of TiO_(2) layer is 0.3μm.The ratio between the edge length of each group of top square holes and the edge length of each group of composite layers is 0.05,the distance between the outside of the SiO_(2) square ring and the outside of the composite layer is 0.1μm,and the width of the square ring is 0.1μm.Figure 3 shows that the ultra-wideband absorption in the wavelength range of 12-52μm,and the polarization insensitivity can be achieved using this absorber.Figure 4 shows that when the TM wave is incident,the angle of incidence increases to 55°in the range of 12-52μm,and the absorptivity can reach approximately 80%.When the TE wave is incident,the angle of incidence increases to 55°in the range of 20-45μm,and the absorptivity reaches approximately 80%.Figure 5 shows that the absorption mechanism of the absorber is surface plasma resonance.The physical mechanism of absorption can also be better understood from the impedance-matching plot(Fig.6).The structural parameters have a substantial impact on the absorption performance.Figure 7 shows the absorptivity curves for different structural parameters and the corresponding magnetic field distribution maps to determine the optimal parameters.Figure 8 shows the absorption spectrum changes with VO_(2) conductivity.Finally,Fig.9 compares the absorption effect of the SiO_(2) pattern in the uppermost layer of each multilayer structure.We determine that,when the SiO_(2) pattern is observed,the absorption bandwidth is wide and the absorption effect is high.Table 1 compares the main performance indicators of the infrared absorber designed for this study and the existing infrared absorber to further demonstrate the superiority of the proposed structure.Conclusions A truncated infrared broadband absorber is designed based on the phase material VO_(2),metalloids,and high-temperature resistance materials NaF and TiO_(2).Using the finite element method,the dependences of the absorptivity on the type of incident wave,angle of incidence,azimuth angle,incident wavelength,and geometric parameters are further analyzed.The results demonstrate that the absorption mechanism of the infrared broadband absorber is the surface plasma resonance effect.When the TM wave is incident,the angle of incidence increases to 55°in the range of 12-52μm,and the absorptivity can reach approximately 80%.When the TE wave is incident,the angle of incidence increases to 55°in the range of 20-45μm,and the absorptivity reaches approximately 80%.When TM or TE waves are incident vertically,three absorption peaks are formed around 14μm,24μm,and 40μm,which are named p1,p2,and p3,respectively.At 21-25μm and 35-43μm,the absorptivity reaches 99.8%;the absorptivity is more than 90%at 12-51μm,the average absorptivity of the broadband absorber reaches 96.4%,and the relative bandwidth reaches 124%.Further,the absorptivity is polarization insensitive.The infrared absorber designed in this study is expected to be widely used in infrared sensing,detection,energy harvesting,and energy conversion.