CN117606619A - Enhanced detection integrated infrared spectrum chip based on tunable surface plasmon - Google Patents
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Abstract
一种基于可调谐表面等离激元的增强探测一体化红外光谱芯片,自上而下依次为源极及漏级、石墨烯/氮化硼异质结、纳米间隙层、介质超表面、电介质层、红外探测器、衬底。其中,介质超表面与石墨烯/氮化硼异质结之间具有纳米间隙层,介质超表面作为栅极,石墨烯/氮化硼异质结表面蒸镀源极及漏级,形成可调谐表面等离激元波导谐振器。红外探测器通过电介质层与可调谐表面等离激元波导谐振器纵向集成,用于红外光谱信号探测。在红外光波照射下,激发低损耗的表面等离激元模式,通过外电场调控谐振峰实现宽波段波长扫描,按时间序列依次获得红外光谱信号,通过处理可获得分子的红外光谱吸收信号,最终实现“光谱增强”与“光谱探测”一体化红外光谱芯片。本发明具有灵敏度高,探测物质种类范围广,体积小,集成度高等优点。
An enhanced detection integrated infrared spectrum chip based on tunable surface plasmons, which from top to bottom is the source and drain stages, graphene/boron nitride heterojunction, nanogap layer, dielectric metasurface, and dielectric layer, infrared detector, substrate. Among them, there is a nanogap layer between the dielectric metasurface and the graphene/boron nitride heterojunction. The dielectric metasurface serves as the gate electrode. The source and drain stages are evaporated on the surface of the graphene/boron nitride heterojunction to form a tunable Surface plasmon waveguide resonators. The infrared detector is vertically integrated with the tunable surface plasmon waveguide resonator through a dielectric layer for infrared spectrum signal detection. Under the irradiation of infrared light waves, the low-loss surface plasmon mode is excited, and the resonant peak is controlled by an external electric field to achieve a wide-band wavelength scan. Infrared spectrum signals are obtained sequentially in a time sequence. Through processing, the infrared spectrum absorption signal of the molecule can be obtained. Finally, Realize the integrated infrared spectrum chip of "spectrum enhancement" and "spectrum detection". The invention has the advantages of high sensitivity, wide range of detection material types, small size and high integration level.
Description
技术领域Technical field
本发明涉及红外光谱技术领域,尤其涉及一种光谱增强与光谱探测一体化红外光谱检测芯片。The invention relates to the technical field of infrared spectroscopy, and in particular to an infrared spectrum detection chip integrating spectrum enhancement and spectrum detection.
背景技术Background technique
红外光谱技术能直接探测分子振动模式,具有高“指纹”特征性、无需样品标记、无损原位检测、定性定量分析等独特优势,是一种极具潜力的现场快速光谱检测技术,广泛应用在生物医疗、环境监测、食品安全检测、化学组成分析、爆炸物检测等关系国计民生及国民经济命脉的重要领域。然而,传统红外光谱技术存在着灵敏度低的难题,其无法检测低浓度的生物分子。其中最主要的原因是中红外光波长(6~16 μm)比分子尺寸(<10 nm)大三个数量级,导致光波与分子相互作用极其微弱,红外光谱信号探测极其困难。Infrared spectroscopy technology can directly detect molecular vibration modes. It has unique advantages such as high "fingerprint" characteristics, no need for sample labeling, non-destructive in-situ detection, and qualitative and quantitative analysis. It is a highly potential on-site rapid spectral detection technology and is widely used in Biomedicine, environmental monitoring, food safety testing, chemical composition analysis, explosive detection and other important fields related to the national economy and people's livelihood and the lifeline of the national economy. However, traditional infrared spectroscopy technology suffers from the problem of low sensitivity and its inability to detect low concentrations of biomolecules. The main reason is that the wavelength of mid-infrared light (6~16 μm) is three orders of magnitude larger than the size of molecules (<10 nm), resulting in extremely weak interaction between light waves and molecules, making it extremely difficult to detect infrared spectrum signals.
近年来,基于表面等离激元效应发展起来的表面增强红外光谱技术能在分子周围激发高度局域的电磁谐振模式,将光波束缚在纳米空间内,从而极大增强光波与分子的相互作用。该技术为解决光波与分子相互作用极其微弱的难题,突破红外光谱系统检测灵敏度低的技术瓶颈提供了一种全新思路,已迅速发展成为了微纳光学、纳米技术、生命科学等前沿交叉领域的研究热点。目前研究高强度的局域电磁模式的激发机理,及其与分子振动模式的相互作用规律,以实现分子红外吸收光谱信号的极大增强是该技术需解决的首要难题。基于国内外研究现状检索,目前主要有以下两种解决思路:In recent years, surface-enhanced infrared spectroscopy technology developed based on the surface plasmon effect can excite highly localized electromagnetic resonance modes around molecules, confining light waves in nanometer space, thereby greatly enhancing the interaction between light waves and molecules. This technology provides a new idea to solve the problem of extremely weak interaction between light waves and molecules, and breaks through the technical bottleneck of low detection sensitivity of infrared spectroscopy systems. It has rapidly developed into a cutting-edge interdisciplinary field such as micro-nano optics, nanotechnology, and life sciences. Research hotspots. Currently, studying the excitation mechanism of high-intensity localized electromagnetic modes and their interaction with molecular vibration modes in order to greatly enhance the molecular infrared absorption spectrum signal is the primary problem that this technology needs to solve. Based on the current research status at home and abroad, there are currently two main solutions:
第一种思路是基于金属表面等离激元效应,采用金属表面等离激元器件与傅里叶红外光谱仪联用的方法实现光谱信号探测。通过设计各种金属纳米结构在分子周围产生高强度的局域电磁模式,对特定种类的痕量分子实现高精度检测。然而,金属表面等离激元谐振频率位于紫外及可见光波段,红外波段金属表面等离激元的能量损耗严重,金属材料的损耗及带宽限制是由金属自由电子气的固有特性所决定,导致其谐振频率无法动态调谐,红外光谱增强波段狭窄。The first idea is based on the metal surface plasmon effect, using a metal surface plasmon device combined with a Fourier transform infrared spectrometer to achieve spectral signal detection. By designing various metal nanostructures to generate high-intensity localized electromagnetic patterns around molecules, high-precision detection of specific types of trace molecules can be achieved. However, the resonant frequency of metal surface plasmons is located in the ultraviolet and visible light bands. The energy loss of metal surface plasmons in the infrared band is serious. The loss and bandwidth limitation of metal materials are determined by the inherent characteristics of metal free electron gas, resulting in The resonant frequency cannot be dynamically tuned, and the infrared spectrum enhancement band is narrow.
第二种思路是基于石墨烯表面等离激元效应增强分子的红外吸收光谱信号,采用表面等离激元器件与傅里叶红外光谱仪联用的方法实现光谱信号探测。二维材料石墨烯是由碳原子构成的一种新型二维晶体材料,能够在红外波段支持表面等离激元本征局域电磁模式,该模式具有损耗极低、局域增强极大、谐振频率可调谐等特性。通过调节外部电压改变石墨烯纳米结构的等离激元频率,可对诸如蛋白质等生物分子的红外振动信息进行高精度的检测。The second idea is to enhance the infrared absorption spectrum signal of molecules based on the graphene surface plasmon effect, and use a surface plasmon device combined with a Fourier transform infrared spectrometer to achieve spectral signal detection. The two-dimensional material graphene is a new two-dimensional crystal material composed of carbon atoms. It can support the surface plasmon intrinsic localized electromagnetic mode in the infrared band. This mode has extremely low loss, large local enhancement, and resonance. Frequency tunable and other features. By adjusting the external voltage to change the plasmon frequency of the graphene nanostructure, the infrared vibration information of biomolecules such as proteins can be detected with high precision.
然而,石墨烯表面等离激元器件仍普遍存在等离激元谐振峰线宽较大,品质因数较低的问题,导致当前的石墨烯表面等离激元增强红外光谱技术存在增强倍数以及光谱分辨力低的难题,使得其通常需要与傅里叶红外光谱仪联用以获得分子的红外吸收光谱信号。由于传统傅里叶红外光谱仪存在体积大、重量大、价格昂贵等缺点,该光谱探测方法对红外光谱仪的严重依赖,严重阻碍了该技术的现场快速检测应用。However, graphene surface plasmon devices still have common problems such as large plasmon resonance peak linewidth and low quality factor, which leads to the existing graphene surface plasmon enhanced infrared spectroscopy technology having enhancement multiples and spectral The problem of low resolution makes it usually necessary to combine it with a Fourier transform infrared spectrometer to obtain the infrared absorption spectrum signal of molecules. Due to the shortcomings of traditional Fourier transform infrared spectrometers such as large size, heavy weight, and high price, this spectral detection method relies heavily on infrared spectrometers, which seriously hinders the rapid on-site detection application of this technology.
发明内容Contents of the invention
本发明为了克服现有技术的不足,提出一种基于可调谐表面等离激元的增强探测一体化红外光谱芯片,采用石墨烯/氮化硼异质结与介质超表面复合,设计可调谐表面等离激元波导谐振器,激发低损耗的表面等离激元模式,实现窄带滤波及分子红外吸收光谱增强;将可调谐表面等离激元波导谐振器与红外探测器单片集成,通过外电场调控谐振峰实现宽波段波长扫描,按时间序列依次获得红外光谱信号,最终实现分子红外吸收光谱信号的增强及探测,具有使用方便,灵敏度高,集成度高,可实现多种未知痕量分子实现探测等优点,可用于生物医疗、环境监测、食品安全等领域。In order to overcome the shortcomings of the existing technology, the present invention proposes an enhanced detection integrated infrared spectrum chip based on tunable surface plasmons, which uses graphene/boron nitride heterojunction and dielectric metasurface composite to design a tunable surface The plasmon waveguide resonator excites low-loss surface plasmon modes to achieve narrow-band filtering and molecular infrared absorption spectrum enhancement; the tunable surface plasmon waveguide resonator and the infrared detector are monolithically integrated, and the external The electric field regulates the resonant peak to achieve wide-band wavelength scanning, and obtains infrared spectrum signals in a time sequence, ultimately realizing the enhancement and detection of molecular infrared absorption spectrum signals. It is easy to use, has high sensitivity and high integration, and can realize a variety of unknown trace molecules. Realizing advantages such as detection, it can be used in fields such as biomedicine, environmental monitoring, and food safety.
为解决本发明的技术问题,所采用的技术方案为:In order to solve the technical problems of the present invention, the technical solutions adopted are:
基于可调谐表面等离激元的增强探测一体化红外光谱芯片,所述芯片自上而下依次设置有源极及漏级、石墨烯/氮化硼异质结、纳米间隙层、介质超表面、电介质层、红外探测器和衬底。An enhanced detection integrated infrared spectrum chip based on tunable surface plasmons. The chip is provided with source and drain stages, graphene/boron nitride heterojunction, nanogap layer, and dielectric metasurface from top to bottom. , dielectric layer, infrared detector and substrate.
所述介质超表面,是通过在电介质层表面沉积硅层,进一步对硅层加工形成超表面的结构轮廓,获得介质超表面结构,用于实现表面等离激元模式与自由空间光的波矢匹配。所述介质超表面同时作为背电极用于实现石墨烯的电学调控。相比于采用金属超表面,使用介质超表面能够有效减少损耗,提高光谱的品质因数(Q值)。The dielectric metasurface is obtained by depositing a silicon layer on the surface of the dielectric layer, and further processing the silicon layer to form the structural outline of the metasurface, thereby obtaining the dielectric metasurface structure, which is used to realize the surface plasmon mode and the wave vector of free space light. match. The dielectric metasurface also serves as a back electrode to achieve electrical control of graphene. Compared with using metal metasurfaces, using dielectric metasurfaces can effectively reduce losses and improve the quality factor (Q value) of the spectrum.
所述石墨烯/氮化硼异质结,是将氮化硼薄膜与石墨烯薄膜复合,用于降低基底对石墨烯材料特性的影响,以获得低损耗表面等离激元模式。The graphene/boron nitride heterojunction is a composite of a boron nitride film and a graphene film, which is used to reduce the influence of the substrate on the graphene material properties to obtain a low-loss surface plasmon mode.
所述介质超表面和所述石墨烯/氮化硼异质结之间具有纳米间隙层,纳米间隙层作为栅极介质层,所述石墨烯/氮化硼异质结与所述介质超表面形成类似于平行板电容结构。There is a nanogap layer between the dielectric metasurface and the graphene/boron nitride heterojunction. The nanogap layer serves as a gate dielectric layer. The graphene/boron nitride heterojunction and the dielectric metasurface Forming a structure similar to a parallel plate capacitor.
所述源极和漏极,沉积在石墨烯/氮化硼异质结上,源极和漏极通过石墨烯导通。The source electrode and the drain electrode are deposited on the graphene/boron nitride heterojunction, and the source electrode and the drain electrode are connected through the graphene.
所述电介质层,位于所述红外探测器裸片和所述介质超表面之间,即位于红外探测器上作为保护层,用于保护红外探测器裸片表面,避免后续微纳加工对红外探测器裸片造成伤害。The dielectric layer is located between the infrared detector die and the dielectric metasurface, that is, it is located on the infrared detector as a protective layer to protect the surface of the infrared detector die and avoid subsequent micro-nano processing of infrared detection. causing damage to the device die.
所述红外探测器位于衬底之上,通过电介质层与所述石墨烯/氮化硼异质结、所述纳米间隙层以及所述介质超表面形成的可调谐表面等离激元波导谐振器纵向单片集成,用于红外光谱信号探测,通过光谱重构算法对探测积分信号进行去噪与解调,获得分子的红外光谱吸收信号,根据所得光谱信息实现对痕量分子的检测。The infrared detector is located on the substrate, and a tunable surface plasmon waveguide resonator is formed by a dielectric layer, the graphene/boron nitride heterojunction, the nanogap layer and the dielectric metasurface. Vertical monolithic integration is used for infrared spectrum signal detection. The detection integrated signal is denoised and demodulated through the spectral reconstruction algorithm to obtain the infrared spectrum absorption signal of the molecule. The detection of trace molecules is realized based on the obtained spectral information.
本发明的以上结构中,所述石墨烯/氮化硼异质结、所述纳米间隙层以及所述介质超表面,形成可调谐表面等离激元波导谐振器,可在红外光波激发下产生可调谐表面等离激元,从而在石墨烯表面产生强局域电场。进一步通过在所述石墨烯/氮化硼异质结和介质超表面之间施加外部电压,对石墨烯的表面电导率进行调节,从而对表面等离激元谐振峰进行动态调节,实现窄带滤波。同时,当表面等离激元谐振频率调谐到与待检测物质的分子振动频率一致时,被测分子周围单位空间内的电磁场强度达到最强,极大增强待测分子的红外光谱信号。In the above structure of the present invention, the graphene/boron nitride heterojunction, the nanogap layer and the dielectric metasurface form a tunable surface plasmon waveguide resonator that can be generated under infrared light wave excitation. Surface plasmons can be tuned to generate strong local electric fields on the graphene surface. Further, by applying an external voltage between the graphene/boron nitride heterojunction and the dielectric metasurface, the surface conductivity of the graphene is adjusted, thereby dynamically adjusting the surface plasmon resonance peak and achieving narrow-band filtering. . At the same time, when the surface plasmon resonance frequency is tuned to be consistent with the molecular vibration frequency of the substance to be detected, the electromagnetic field intensity in the unit space around the molecule to be detected reaches its strongest, greatly enhancing the infrared spectrum signal of the molecule to be detected.
优选地,在所述石墨烯/氮化硼异质结和介质超表面之间施加的外部电压范围为-2~2V,对石墨烯表面等离激元谐振峰在5~16μm红外范围内实现动态调节。Preferably, the external voltage applied between the graphene/boron nitride heterojunction and the dielectric metasurface ranges from -2 to 2 V, and the graphene surface plasmon resonance peak is achieved in the infrared range of 5 to 16 μm. Dynamic adjustment.
采用本发明上述结构器件,在不同电压条件下探测到电信号,并将探测到的信号形成对应集合,构建数值计算模型并将其转化成线性模型,通过优化算法得到待解参数,并根据最优值重构光谱信息实现对红外探测器输出的探测积分信号进行去噪与解调,获得分子的红外光谱吸收信号。根据所得光谱信息实现对痕量分子的检测。Using the above-mentioned structural device of the present invention, electrical signals are detected under different voltage conditions, and the detected signals are formed into corresponding sets. A numerical calculation model is constructed and converted into a linear model. The parameters to be solved are obtained through an optimization algorithm, and based on the optimal The value of excellence reconstructs spectral information to denoise and demodulate the integrated detection signal output by the infrared detector to obtain the infrared spectrum absorption signal of the molecule. The detection of trace molecules is achieved based on the obtained spectral information.
进一步地,所述介质超表面的超表面结构采用周期性阵列结构,在芯片的横切方向上呈矩形、圆形、蝴蝶结形、双蝴蝶结形、同心环型或十字架形等不同结构形状,可以通过电子束曝光、聚焦离子束刻蚀、紫外光刻、激光直写等光刻技术,结合电子束蒸镀、磁控溅射、热蒸镀等方法得到,超表面结构的尺寸和周期范围为0.1μm~1μm,超表面结构的厚度范围为20~100nm。Furthermore, the metasurface structure of the dielectric metasurface adopts a periodic array structure, and has different structural shapes such as rectangle, circle, bowtie shape, double bowtie shape, concentric ring shape or cross shape in the transverse direction of the chip. It is obtained through photolithography technologies such as electron beam exposure, focused ion beam etching, ultraviolet lithography, and laser direct writing, combined with methods such as electron beam evaporation, magnetron sputtering, and thermal evaporation. The size and period range of the metasurface structure is 0.1μm~1μm, and the thickness of the metasurface structure ranges from 20~100nm.
进一步地,所述石墨烯/氮化硼异质结,是将氮化硼薄膜与石墨烯薄膜在垂直方向上多层叠加,叠加层数为1~5层,氮化硼位于异质结底层与纳米间隙层接触,石墨烯位于异质结顶层,与源极漏极接触导通,可以通过机械剥离工艺或者化学气相沉积法制备获得,所述异质结薄膜的层数可以通过多次转移方式实现。Further, the graphene/boron nitride heterojunction is a multi-layer stack of boron nitride films and graphene films in the vertical direction. The number of stacked layers is 1 to 5, and boron nitride is located at the bottom layer of the heterojunction. In contact with the nanogap layer, graphene is located on the top layer of the heterojunction and is in contact with the source and drain. It can be prepared through a mechanical peeling process or a chemical vapor deposition method. The number of layers of the heterojunction film can be transferred through multiple transfers. way to achieve.
进一步地,所述位于石墨烯/氮化硼异质结与介质超表面间的纳米间隙层,厚度范围为2-20nm, 材料为红外透明材料,选自:Al2O3,KBr,MgF2,CaF2,BaF2,AgCl,ZnSe,SiO2。Further, the nanogap layer located between the graphene/boron nitride heterojunction and the dielectric metasurface has a thickness range of 2-20nm, and the material is an infrared transparent material selected from: Al 2 O 3 , KBr, MgF 2 , CaF 2 , BaF 2 , AgCl, ZnSe, SiO 2 .
进一步地,所述位于红外探测器上电介质层的厚度范围为100-500nm,用于保护红外探测器裸片,所述电介质层的材料为红外透明材料,选自:Al2O3,KBr,MgF2,CaF2,BaF2,AgCl,ZnSe,SiO2。Further, the thickness of the dielectric layer on the infrared detector ranges from 100 to 500 nm, which is used to protect the infrared detector bare chip. The material of the dielectric layer is an infrared transparent material, selected from: Al 2 O 3 , KBr, MgF 2 , CaF 2 , BaF 2 , AgCl, ZnSe, SiO 2 .
相对于现有技术,本发明具有如下优点:Compared with the existing technology, the present invention has the following advantages:
第一,石墨烯是单层碳原子构成的二维电子气材料,在红外波段支持表面等离激元的传播,通过调节其谐振波长与待测分子的振动频率相一致,可以极大增加痕量分子与光的相互作用。同时,石墨烯具有很大的比表面积和很好的生物兼容性,能够有效地将生物分子吸附在石墨烯表面。First, graphene is a two-dimensional electron gas material composed of a single layer of carbon atoms. It supports the propagation of surface plasmons in the infrared band. By adjusting its resonant wavelength to be consistent with the vibration frequency of the molecule to be measured, the trace can be greatly increased. The interaction of light molecules with light. At the same time, graphene has a large specific surface area and good biocompatibility, and can effectively adsorb biomolecules on the surface of graphene.
第二,本发明利用石墨烯/氮化硼异质结与介质超表面复合的方式,有效避免了石墨烯纳米图形化引入的大量边界和缺陷,提升石墨烯自由载流子的寿命,从而提升石墨烯表面等离激元的寿命,有效降低光学损耗。与如图5所示,采用石墨烯/氮化硼异质结后能够激发更低低损耗的表面等离激元模式,获得激发效率更高线宽更窄的等离激元谐振峰,从而能够在应用时提高表面等离激元谐振模式与分子振动模式的耦合效率,提升检测灵敏度。Second, the present invention utilizes the composite method of graphene/boron nitride heterojunction and dielectric metasurface to effectively avoid a large number of boundaries and defects introduced by graphene nanopatterning, improve the lifetime of graphene free carriers, and thereby enhance The lifetime of graphene surface plasmons effectively reduces optical losses. As shown in Figure 5, the use of graphene/boron nitride heterojunction can excite a lower and low-loss surface plasmon mode, and obtain a plasmon resonance peak with higher excitation efficiency and narrower line width. It can improve the coupling efficiency between the surface plasmon resonance mode and the molecular vibration mode during application, and improve the detection sensitivity.
第三,本发明设计的石墨烯/氮化硼异质结、纳米间隙层以及介质超表面三者复合形成可调谐等离激元波导谐振器,能够获得线宽更窄的等离激元谐振峰,通过施加外部偏置电压实现对石墨烯表面电导率的调节,能够对石墨烯表面等离激元谐振波长进行宽波段动态调谐,以实现红外波段的窄带滤波。Third, the graphene/boron nitride heterojunction, nanogap layer and dielectric metasurface designed in the present invention are combined to form a tunable plasmon waveguide resonator, which can obtain plasmon resonance with a narrower line width. Peak, by applying an external bias voltage to adjust the conductivity of the graphene surface, it is possible to perform wide-band dynamic tuning of the graphene surface plasmon resonance wavelength to achieve narrow-band filtering in the infrared band.
第四,现有的石墨烯表面等离激元通常需要与傅里叶红外光谱仪联用以获得分子的红外吸收光谱信号,由于传统傅里叶红外光谱仪存在体积大、重量大、价格昂贵等缺点,阻碍了该技术从实验室抽样分析走向现场快速检测。为了解决该难题,本发明提出了可调谐表面等离激元波导谐振器与红外探测器单片集成结构,不依赖传统光学干涉结构、频率扫描及分光部件,构建增强及探测一体化红外光谱芯片,极大增强分子红外吸收光谱信号,在同一器件上实现“光谱增强”及“光谱探测”。本发明可以通过外电场调控谐振器谐振峰实现波长扫描,通过光谱重构算法对探测积分信号进行去噪与解调,获得分子的红外光谱吸收信号,即可实现分子检测,无需使用传统傅里叶红外光谱仪,可面向现场快速检测。Fourth, existing graphene surface plasmons usually need to be used in conjunction with a Fourier transform infrared spectrometer to obtain the infrared absorption spectrum signal of molecules. Due to the shortcomings of traditional Fourier transform infrared spectrometers, such as large size, heavy weight, and high price, , hindering the technology from moving from laboratory sampling analysis to on-site rapid detection. In order to solve this problem, the present invention proposes a monolithic integrated structure of a tunable surface plasmon waveguide resonator and an infrared detector. It does not rely on traditional optical interference structures, frequency scanning and spectroscopic components to build an enhanced and detected integrated infrared spectrum chip. , greatly enhances the molecular infrared absorption spectrum signal, and achieves "spectral enhancement" and "spectral detection" on the same device. This invention can achieve wavelength scanning by regulating the resonant peak of the resonator through an external electric field, denoise and demodulate the detection integrated signal through a spectrum reconstruction algorithm, and obtain the infrared spectrum absorption signal of the molecule, thereby realizing molecule detection without using traditional Fourier methods. Leaf infrared spectrometer can be used for rapid on-site detection.
可见,本发明能够同时实现分子红外吸收信号的“光谱增强”及“光谱探测”,并具有灵敏度高,宽波段动态可调谐,体积小,易集成等优点,具有广泛的应用前景。It can be seen that the present invention can realize "spectral enhancement" and "spectral detection" of molecular infrared absorption signals at the same time, and has the advantages of high sensitivity, wide band dynamic tunability, small size, easy integration, etc., and has broad application prospects.
附图说明Description of drawings
图1为增强探测一体化红外光谱芯片示意图;Figure 1 is a schematic diagram of the enhanced detection integrated infrared spectrum chip;
图2(a)-图2(f)为矩形、圆形、蝴蝶结形、双蝴蝶结形、同心环型或十字架形的介质超表面的天线阵列示意图;Figure 2(a)-Figure 2(f) are schematic diagrams of antenna arrays of rectangular, circular, bowtie-shaped, double bowtie-shaped, concentric ring-shaped or cross-shaped dielectric metasurfaces;
图3介质超表面的纵向剖面放大图;Figure 3 is an enlarged longitudinal cross-section of the dielectric metasurface;
图4为增强探测一体化红外光谱芯片的制备方法流程图;Figure 4 is a flow chart of the preparation method of the enhanced detection integrated infrared spectrum chip;
图5为石墨烯/氮化硼异质结与不同石墨烯电子弛豫时间下红外吸收光谱;Figure 5 shows the infrared absorption spectrum of graphene/boron nitride heterojunction and different graphene electronic relaxation times;
图6不同电压条件下增强探测一体化红外光谱芯片的红外吸收光谱;Figure 6 Infrared absorption spectrum of enhanced detection integrated infrared spectrum chip under different voltage conditions;
图7为增强探测一体化红外光谱芯片吸附探针分子后的重构红外光谱信号;Figure 7 shows the reconstructed infrared spectrum signal after the enhanced detection integrated infrared spectrum chip adsorbs probe molecules;
图8为增强探测一体化红外光谱芯片检测的分子红外吸收光谱;Figure 8 shows the molecular infrared absorption spectrum detected by the enhanced detection integrated infrared spectrum chip;
具体实施方式Detailed ways
为了使本发明的目的、技术方案及优点更加清楚明白,下面结合附图对本发明的优选实例作进一步详细描述,附图中相同的标记代表相同或类似的部件。In order to make the purpose, technical solutions and advantages of the present invention more clear, the preferred embodiments of the present invention will be described in further detail below in conjunction with the accompanying drawings, in which the same symbols represent the same or similar components.
参见图1,本发明设计的基于可调谐表面等离激元的增强探测一体化红外光谱芯片包括自下而上依次设置的衬底1、红外探测器2、电介质层3、介质超表面4、纳米间隙层5、石墨烯/氮化硼异质结6、源极7及漏极8。测试时,待测分子10通过喷涂、旋涂、滴涂等方式置于所述芯片上。其中,红外探测器2位于衬底1上,电介质层3位于红外探测器2上,介质超表面4同时作为栅极位于电介质层3上,石墨烯/氮化硼异质结6位于纳米间隙层5上,源极7和漏极8沉积在石墨烯/氮化硼异质结6上,源极7和漏极8通过石墨烯/氮化硼异质结6导通。Referring to Figure 1, the enhanced detection integrated infrared spectrum chip based on tunable surface plasmons designed by the present invention includes a substrate 1, an infrared detector 2, a dielectric layer 3, a dielectric metasurface 4, and a substrate 1 arranged in sequence from bottom to top. Nanogap layer 5, graphene/boron nitride heterojunction 6, source electrode 7 and drain electrode 8. During testing, the molecules 10 to be tested are placed on the chip through spraying, spin coating, drop coating, etc. Among them, the infrared detector 2 is located on the substrate 1, the dielectric layer 3 is located on the infrared detector 2, the dielectric metasurface 4 serves as a gate electrode and is located on the dielectric layer 3, and the graphene/boron nitride heterojunction 6 is located on the nanogap layer 5, the source electrode 7 and the drain electrode 8 are deposited on the graphene/boron nitride heterojunction 6, and the source electrode 7 and the drain electrode 8 are conductive through the graphene/boron nitride heterojunction 6.
以上结构中,将纳米间隙层5设置于介质超表面4以及石墨烯/氮化硼异质结6中间,构成可调谐表面等离激元波导谐振器,用于激发红外波段表面等离激元,同时形成类似于平行板电容结构,通过在石墨烯/氮化硼异质结6和介质超表面4之间通过电压源9施加外部电压,对石墨烯的费米能级进行调控,实现等离激元谐振峰的调控。纳米间隙层5的厚度范围为2-20nm,材料为红外透明材料,可选自:Al2O3,KBr,MgF2,CaF2,BaF2,AgCl,ZnSe,SiO2。In the above structure, the nanogap layer 5 is arranged between the dielectric metasurface 4 and the graphene/boron nitride heterojunction 6 to form a tunable surface plasmon waveguide resonator for exciting surface plasmons in the infrared band. , and at the same time, a structure similar to a parallel plate capacitor is formed. By applying an external voltage through the voltage source 9 between the graphene/boron nitride heterojunction 6 and the dielectric metasurface 4, the Fermi level of graphene is regulated and achieved. Regulation of ionotropic resonance peaks. The thickness of the nanogap layer 5 ranges from 2 to 20 nm, and the material is an infrared transparent material, which can be selected from: Al 2 O 3 , KBr, MgF 2 , CaF 2 , BaF 2 , AgCl, ZnSe, and SiO 2 .
电介质层3位于红外探测器2上,用于阻隔介质超表面4和红外探测器2的直接接触,保护红外探测器2裸片。电介质层3的厚度范围为100~500nm,材料为红外透明材料,可选自:Al2O3,KBr,MgF2,CaF2,BaF2,AgCl,ZnSe,SiO2。The dielectric layer 3 is located on the infrared detector 2 and is used to block direct contact between the dielectric metasurface 4 and the infrared detector 2 and protect the bare chip of the infrared detector 2. The thickness of the dielectric layer 3 ranges from 100 to 500 nm, and the material is an infrared transparent material, which can be selected from: Al 2 O 3 , KBr, MgF 2 , CaF 2 , BaF 2 , AgCl, ZnSe, and SiO 2 .
红外探测器2通过真空镀膜、分子束外延方法制备在衬底1上,可选用的探测器类型包括碲镉汞(HgCdTe)红外探测器、II型超晶格红外探测器、热释电红外探测器,金属电极由真空热蒸发方法制备。通过金属电极加引线的方法将红外探测器和外接电路连接。这样,红外探测器2通过电介质层3与可调谐表面等离激元波导谐振器纵向集成,用于红外光谱信号探测,通过光谱重构算法对探测积分信号进行去噪与解调,获得分子的红外光谱吸收信号,根据所得光谱信息实现对痕量分子的检测。The infrared detector 2 is prepared on the substrate 1 through vacuum coating and molecular beam epitaxy. The available detector types include mercury cadmium telluride (HgCdTe) infrared detector, type II superlattice infrared detector, and pyroelectric infrared detection. device, and the metal electrodes are prepared by vacuum thermal evaporation method. Connect the infrared detector to the external circuit through metal electrodes and leads. In this way, the infrared detector 2 is vertically integrated with the tunable surface plasmon waveguide resonator through the dielectric layer 3 for infrared spectrum signal detection. The detection integrated signal is denoised and demodulated through the spectrum reconstruction algorithm to obtain the molecular information. The infrared spectrum absorbs the signal and realizes the detection of trace molecules based on the obtained spectral information.
参见图2与图3,介质超表面4的结构形状可以采用多种形状,包含图2(a)矩形、2(b)圆形、2(c)蝴蝶结形、2(d)双蝴蝶结形、2(e)同心环型或2(f)十字架形等,这些天线结构的尺寸和周期范围为0.1μm~1μm,厚度范围为20~100nm,可以通过电子束曝光、聚焦离子束刻蚀、紫外光刻、激光直写等光刻技术,结合电子束蒸镀、磁控溅射、热蒸镀等方法制备得到。Referring to Figures 2 and 3, the structural shape of the dielectric metasurface 4 can adopt a variety of shapes, including Figure 2 (a) rectangle, 2 (b) circle, 2 (c) bow tie shape, 2 (d) double bow tie shape, 2(e) concentric ring type or 2(f) cross type, etc. The size and period of these antenna structures range from 0.1μm to 1μm, and the thickness ranges from 20 to 100nm. They can be processed by electron beam exposure, focused ion beam etching, ultraviolet It is prepared using lithography technologies such as photolithography and laser direct writing, combined with methods such as electron beam evaporation, magnetron sputtering, and thermal evaporation.
本发明在石墨烯/氮化硼异质结6与介质超表面4夹着纳米间隙层5,通过介质超表面4在石墨烯/氮化硼异质结6中激发表面等离激元,能够在石墨烯/氮化硼异质结6中石墨烯表面产生强局域电场,该强局域电场与分子振动模式发生耦合,极大增强芯片表面待测分子10的红外吸收信号。In the present invention, a nanogap layer 5 is sandwiched between the graphene/boron nitride heterojunction 6 and the dielectric metasurface 4, and surface plasmons are excited in the graphene/boron nitride heterojunction 6 through the dielectric metasurface 4, so that In the graphene/boron nitride heterojunction 6, a strong local electric field is generated on the graphene surface, and the strong local electric field is coupled with the molecular vibration mode, greatly enhancing the infrared absorption signal of the molecules to be measured 10 on the chip surface.
图4为制备增强探测一体化红外光谱芯片的详细加工流程图:Figure 4 is a detailed processing flow chart for preparing an integrated infrared spectrum chip for enhanced detection:
步骤S1,制备红外探测器:利用真空镀膜、分子束外延和真空热蒸发方法在衬底1上制备红外敏感材料薄膜,制备红外探测器2。Step S1, prepare an infrared detector: use vacuum coating, molecular beam epitaxy and vacuum thermal evaporation methods to prepare an infrared sensitive material film on the substrate 1 to prepare an infrared detector 2.
步骤S2,制备电介质层:利用电子束蒸镀、原子沉积或分子束外延生长的方法在红外探测器表面制备电介质作为电介质层3,用作保护层。Step S2, prepare a dielectric layer: use electron beam evaporation, atomic deposition or molecular beam epitaxial growth to prepare a dielectric as dielectric layer 3 on the surface of the infrared detector, which is used as a protective layer.
步骤S3,制备介质超表面4:采用利用磁控溅射、电子束蒸镀、原子沉积等方式在电介质层3表面沉积硅层,利用电子束曝光或聚焦离子束刻蚀的方法在电所沉积的硅层上刻写超表面的结构轮廓,对电子束曝光结构进行干法刻蚀获得介质超表面结构4,同时将该介质超表面作为栅极。Step S3, prepare the dielectric metasurface 4: deposit a silicon layer on the surface of the dielectric layer 3 using magnetron sputtering, electron beam evaporation, atomic deposition, etc., and use electron beam exposure or focused ion beam etching to deposit the silicon layer on the surface of the dielectric layer 3 The structural outline of the metasurface is written on the silicon layer, and the electron beam exposed structure is dry-etched to obtain the dielectric metasurface structure 4, and the dielectric metasurface is used as a gate electrode.
步骤S4,制备纳米间隙层:利用磁控溅射、电子束蒸镀、原子沉积的方法在介质超表面上制备电介质作为纳米间隙层5,以实现表面等离激元激发及栅极电压调控。Step S4, prepare the nanogap layer: use magnetron sputtering, electron beam evaporation, and atomic deposition to prepare a dielectric as the nanogap layer 5 on the dielectric metasurface to achieve surface plasmon excitation and gate voltage regulation.
步骤S5,制备氮化硼薄膜:利用机械剥离工艺或者化学气相沉积法制备氮化硼薄膜;Step S5, prepare a boron nitride film: use a mechanical peeling process or a chemical vapor deposition method to prepare a boron nitride film;
步骤S6,制备石墨烯薄膜:利用机械剥离工艺或者化学气相沉积法制备石墨烯薄膜;Step S6, prepare a graphene film: prepare a graphene film using a mechanical peeling process or a chemical vapor deposition method;
步骤S7,转移石墨烯/氮化硼异质结薄膜:将制备得到的氮化硼薄膜和石墨烯薄膜,依次交替叠加转移到上述制备得到的基底上,转移时氮化硼位于异质结底层与纳米间隙层接触,石墨烯位于异质结顶层,与源极漏极接触导通。所述石墨烯/氮化硼异质结薄膜6的层数为1~5层,多层结构可以通过多次转移方式实现。Step S7, transfer the graphene/boron nitride heterojunction film: the prepared boron nitride film and the graphene film are alternately stacked and transferred to the substrate prepared above. During the transfer, the boron nitride is located at the bottom layer of the heterojunction. In contact with the nanogap layer, graphene is located on the top layer of the heterojunction and is in contact with the source and drain electrodes. The number of layers of the graphene/boron nitride heterojunction film 6 is 1 to 5, and the multi-layer structure can be realized through multiple transfers.
步骤S8,制备源极和漏极:利用紫外光刻、激光直写、电子束蒸镀在石墨烯/氮化硼异质结薄膜6上制备金属接触欧姆电极,即源极7和漏极8。Step S8, prepare the source and drain electrodes: use ultraviolet lithography, laser direct writing, and electron beam evaporation to prepare metal contact ohmic electrodes, namely the source electrode 7 and the drain electrode 8, on the graphene/boron nitride heterojunction film 6 .
所述介质超表面4、纳米间隙层5、石墨烯/氮化硼异质结6所构成的可调谐表面等离激元波导谐振器可以在红外光波激发下产生表面等离激元,从而在红外区域产生强烈的吸收,如图3所示,从而在石墨烯表面产生强局域电场;进一步通过在所述介质超表面4和石墨烯/氮化硼异质结6之间施加外部电压9,对石墨烯的表面电导率进行调节。所述的外界电压9范围为-2~2V,对石墨烯/氮化硼异质结6的表面等离激元谐振峰在5~16μm红外范围内的动态调节。The tunable surface plasmon waveguide resonator composed of the dielectric metasurface 4, nanogap layer 5, and graphene/boron nitride heterojunction 6 can generate surface plasmons under infrared light wave excitation, thereby The infrared region produces strong absorption, as shown in Figure 3, thereby generating a strong local electric field on the graphene surface; further by applying an external voltage 9 between the dielectric metasurface 4 and the graphene/boron nitride heterojunction 6 , to adjust the surface conductivity of graphene. The external voltage 9 ranges from -2 to 2V, and dynamically adjusts the surface plasmon resonance peak of the graphene/boron nitride heterojunction 6 in the infrared range of 5 to 16 μm.
如图8所示,随着外部电压从-0.5V增加到-2V,对应的增强谐振峰发生蓝移;当激发的石墨烯表面等离激元谐振频率调谐到与待检测分子10的分子振动频率相一致时,被测分子周围单位空间内的电磁场强度达到最强,从而增强待测分子10的红外光谱信号。As shown in Figure 8, as the external voltage increases from -0.5V to -2V, the corresponding enhanced resonance peak undergoes a blue shift; when the excited graphene surface plasmon resonance frequency is tuned to be consistent with the molecular vibration of the molecule to be detected 10 When the frequencies are consistent, the electromagnetic field intensity in the unit space around the molecule to be measured reaches the strongest, thereby enhancing the infrared spectrum signal of the molecule to be measured 10 .
该光谱信号进一步被红外探测器2所探测,得到不同电压条件下探测的电信号。通过光谱重构算法实现对红外探测器输出的探测积分信号的去噪与解调,图6与图7分别为吸附探针分子前后的重构红外光谱信号,最终获得待测分子10的红外光谱吸收信号,根据所得光谱信息实现对痕量分子的检测。The spectral signal is further detected by the infrared detector 2, and electrical signals detected under different voltage conditions are obtained. The spectral reconstruction algorithm is used to denoise and demodulate the detection integrated signal output by the infrared detector. Figure 6 and Figure 7 show the reconstructed infrared spectrum signal before and after adsorption of the probe molecule respectively. Finally, the infrared spectrum of the molecule to be measured 10 is obtained. The absorption signal is used to detect trace molecules based on the obtained spectral information.
下面进一步结合实施例对本发明的实现原理和预期效果进行阐述。然而,本发明并不受限于以下公开的示范性实施例,相关领域技术人员可以通过不同形式来对其加以实现。说明书的实质仅仅是帮助相关领域技术人员综合理解本发明的具体细节。The implementation principles and expected effects of the present invention will be further described below with reference to embodiments. However, the present invention is not limited to the exemplary embodiments disclosed below, and those skilled in the relevant art can implement it in different forms. The essence of the description is only to help those skilled in the relevant fields comprehensively understand the specific details of the present invention.
本实施例以基于HgCdTe探测器的石墨烯等离激元增强探测一体化芯片为例,首先利用真空镀膜、分子外延的方法在衬底上生长一层HgCdTe材料,制备红外探测器,并将其接入外部电路;其次利用电子束蒸镀的方法红外探测器表面沉积一层厚度约为200 nm的氧化铝膜,作为电介质层保护红外探测器;然后通过磁控溅射工艺在电介质层上沉积一层厚度约为30 nm的硅,用作栅极材料调控石墨烯的费米能级和载流子浓度,同时用作介质超表面材料;再利用聚焦离子束刻蚀工艺制备介质超表面结构,介质超表面结构形状为蝴蝶结型,周期为300nm,间隙为80 nm,超表面的整体尺寸为100 μm×100 μm;接着利用原子层沉积的方法在介质超表面结构上沉积厚度约为10 nm的薄层氧化铝,制备纳米间隙层;进一步采用化学气相沉积(CVD)分别在铜箔上生长单层氮化硼(0.1 nm)及单层石墨烯(0.34nm)薄膜,并使用聚(甲基丙烯酸甲酯)(PMMA)作为转移试剂将氮化硼薄膜和石墨烯薄膜依次叠加转移到薄层氧化铝上;最后,利用紫外光刻蚀及电子束蒸镀在石墨烯/氮化硼异质结上制备金源极和漏极。This embodiment takes the graphene plasmon enhanced detection integrated chip based on HgCdTe detector as an example. First, vacuum coating and molecular epitaxy are used to grow a layer of HgCdTe material on the substrate to prepare an infrared detector, and then Connect to an external circuit; secondly, use electron beam evaporation to deposit an aluminum oxide film with a thickness of about 200 nm on the surface of the infrared detector as a dielectric layer to protect the infrared detector; then deposit it on the dielectric layer through a magnetron sputtering process A layer of silicon with a thickness of about 30 nm is used as a gate material to control the Fermi level and carrier concentration of graphene, and is also used as a dielectric metasurface material; the focused ion beam etching process is then used to prepare the dielectric metasurface structure. , the shape of the dielectric metasurface structure is a bow tie, the period is 300nm, the gap is 80 nm, and the overall size of the metasurface is 100 μm × 100 μm; then the atomic layer deposition method is used to deposit a thickness of about 10 nm on the dielectric metasurface structure A thin layer of aluminum oxide was used to prepare a nanogap layer; chemical vapor deposition (CVD) was further used to grow a single layer of boron nitride (0.1 nm) and a single layer of graphene (0.34nm) films on the copper foil, and poly(methane) was used. Using methyl acrylate (PMMA) as a transfer reagent, the boron nitride film and the graphene film are sequentially superimposed and transferred to a thin layer of alumina; finally, ultraviolet photolithography and electron beam evaporation are used to coat the graphene/boron nitride heterogeneous Gold source and drain electrodes were prepared on the junction.
由于探测器表面处的晶格缺陷、机械损伤和杂质污染都可能在禁带中引入能级,使得表面陷阱电荷密度增加,产生更多的表面复合,更多的注入载流子在表面复合消失,严重影响器件性能。因此,红外探测器集成工艺的难点在于如何优化器件表面钝化工艺,通过在半导体表面沉积或生长一层合适的钝化薄膜,进而束缚半导体表面的悬挂键,降低表面态密度,减小表面的复合速率,有效降低器件暗电流,提高探测性能。Since lattice defects, mechanical damage and impurity contamination on the surface of the detector may introduce energy levels in the forbidden band, the surface trap charge density increases, resulting in more surface recombination, and more injected carriers recombine and disappear on the surface. , seriously affecting device performance. Therefore, the difficulty of the infrared detector integration process is how to optimize the device surface passivation process. By depositing or growing a suitable passivation film on the semiconductor surface, it can bind the dangling bonds on the semiconductor surface, reduce the surface state density, and reduce the surface The recombination rate effectively reduces device dark current and improves detection performance.
实施例采用生物分子作为探针分子,在探测芯片上旋涂8nm厚的生物分子薄膜。图8为不同电压条件下芯片对生物分子的红外吸收增强曲线。从图中可以看出,生物分子在6.235μm及6.355μm处的振动模式在石墨烯纳米探针上被极大增强。通过控制外部电压从-0.5V增加到-2V使石墨烯纳米探针的红外谐振频率发生蓝移,可以对生物分子振动模式进行选择性增强。从图中可以看出,生物分子振动模式与石墨烯表面等离激元谐振模式耦合引起凹陷峰,其频率对应生物分子各个振动模式的谐振频率。在外电压为-0.5V及-2V时,石墨烯纳米探针谐振模式与生物分子振动频率最接近,此时分子振动模式的增强效果最大。计算得到芯片对生物分子红外光谱信号的增强因子最高可达100倍。In the embodiment, biomolecules are used as probe molecules, and an 8 nm thick biomolecule film is spin-coated on the detection chip. Figure 8 shows the infrared absorption enhancement curves of the chip for biomolecules under different voltage conditions. It can be seen from the figure that the vibration modes of biomolecules at 6.235μm and 6.355μm are greatly enhanced on the graphene nanoprobe. By controlling the external voltage to increase from -0.5V to -2V to blue-shift the infrared resonance frequency of the graphene nanoprobe, the vibration mode of biomolecules can be selectively enhanced. It can be seen from the figure that the coupling of the biomolecule vibration mode and the graphene surface plasmon resonance mode causes a concave peak, whose frequency corresponds to the resonance frequency of each vibration mode of the biomolecule. When the external voltage is -0.5V and -2V, the resonance mode of the graphene nanoprobe is closest to the vibration frequency of biomolecules, and the enhancement effect of the molecular vibration mode is greatest at this time. It is calculated that the chip can enhance the infrared spectrum signal of biomolecules by up to 100 times.
最后说明的是,以上实施例仅用于说明本发明的技术方案而非限制,尽管通过上述实施例已经对本发明进行了详细的描述,但是本领域技术人员应当理解,说明和实施例仅被认为是示例性的,可以在形式上和细节上做出各式各样的变化,本发明的真正范围和主旨均由权利要求所限定。Finally, it should be noted that the above embodiments are only used to illustrate the technical solutions of the present invention and are not limiting. Although the present invention has been described in detail through the above embodiments, those skilled in the art should understand that the illustrations and examples are only considered to be are illustrative and may be variously changed in form and detail. The true scope and spirit of the invention are defined by the claims.
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