CN104568809A - Intermediate infrared molecular vibration spectrum sensing method based on graphene array structure - Google Patents
Intermediate infrared molecular vibration spectrum sensing method based on graphene array structure Download PDFInfo
- Publication number
- CN104568809A CN104568809A CN201510053031.8A CN201510053031A CN104568809A CN 104568809 A CN104568809 A CN 104568809A CN 201510053031 A CN201510053031 A CN 201510053031A CN 104568809 A CN104568809 A CN 104568809A
- Authority
- CN
- China
- Prior art keywords
- mid
- array structure
- graphene
- infrared
- graphene array
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
本发明属于检测技术领域,具体涉及一种基于石墨烯阵列结构的中红外分子振动谱传感方法,包括以下步骤:A.提供中红外频段场与物质相互作用的石墨烯阵列结构,由石墨烯周期阵列附着于基底介质层上构成,被中红外平行波束垂直照射;B1.对于液态化学物质的检测,在石墨烯阵列结构上覆盖一层待测样品;B2.对于气态化学物质的检测,将石墨烯阵列结构放置于一个封闭的腔体中,通入待测气体;C.波长可调的中红外光源通过透镜变换为平行波束,垂直照射激励石墨烯阵列结构,采用检测阵列检测,得到表征待测样品分子振动特征的传输谱,以此获得分子振动谱。发明有利于发展简易、实时的分子振动谱测量仪器。
The invention belongs to the technical field of detection, and specifically relates to a mid-infrared molecular vibration spectrum sensing method based on a graphene array structure, comprising the following steps: A. providing a graphene array structure for the interaction between a mid-infrared frequency band field and a substance, composed of graphene The periodic array is attached to the base medium layer and is vertically irradiated by the mid-infrared parallel beam; B1. For the detection of liquid chemical substances, a layer of sample to be tested is covered on the graphene array structure; B2. For the detection of gaseous chemical substances, the The graphene array structure is placed in a closed cavity, and the gas to be measured is passed through; C. The mid-infrared light source with adjustable wavelength is transformed into a parallel beam through the lens, and the graphene array structure is excited by vertical irradiation, and the detection array is used to detect and obtain the characterization The transmission spectrum of the molecular vibration characteristics of the sample to be measured is used to obtain the molecular vibration spectrum. The invention is conducive to the development of simple and real-time molecular vibration spectrum measuring instruments.
Description
技术领域technical field
本发明属于检测技术领域,具体涉及一种基于石墨烯阵列结构的中红外分子振动谱传感方法。The invention belongs to the technical field of detection, and in particular relates to a mid-infrared molecular vibration spectrum sensing method based on a graphene array structure.
背景技术Background technique
中红外分子振动谱广泛应用于化合物分子结构的测定、未知物鉴定以及混合成分分析,是传感识别物质性质和特征的重要参数,也被称为分子振动指纹。目前,采用红外光谱仪可以获得分子振动谱,但是红外光谱仪复杂、价格昂贵。Mid-infrared molecular vibrational spectroscopy is widely used in the determination of the molecular structure of compounds, the identification of unknowns, and the analysis of mixed components. It is an important parameter for sensing and identifying the properties and characteristics of substances, also known as molecular vibrational fingerprints. At present, the molecular vibration spectrum can be obtained by using an infrared spectrometer, but the infrared spectrometer is complex and expensive.
发明内容Contents of the invention
针对红外光谱仪复杂、价格昂贵的问题,本发明提供一种成本低且易于实施的基于石墨烯阵列结构的中红外分子振动谱传感方法。Aiming at the problems of complex and expensive infrared spectrometers, the present invention provides a low-cost and easy-to-implement method for sensing mid-infrared molecular vibrational spectra based on a graphene array structure.
本发明的技术方案是这样实现的:一种基于石墨烯阵列结构的中红外分子振动谱传感方法,包括以下步骤:The technical scheme of the present invention is achieved in that a kind of mid-infrared molecular vibration spectrum sensing method based on graphene array structure comprises the following steps:
A.提供中红外频段场与物质相互作用的石墨烯阵列结构,由石墨烯周期阵列附着于基底介质层上构成,被中红外平行波束垂直照射;A. The graphene array structure that provides the interaction between the mid-infrared frequency field and the substance is composed of a graphene periodic array attached to the base dielectric layer, and is vertically irradiated by the mid-infrared parallel beam;
B1.对于液态化学物质的检测,在石墨烯阵列结构上覆盖一层待测样品;B1. For the detection of liquid chemical substances, a layer of the sample to be tested is covered on the graphene array structure;
B2.对于气态化学物质的检测,将石墨烯阵列结构放置于一个封闭的腔体中,通入待测气体;B2. For the detection of gaseous chemical substances, the graphene array structure is placed in a closed cavity, and the gas to be tested is introduced;
C.波长可调的中红外光源通过透镜变换为平行波束,垂直照射激励石墨烯阵列结构,采用检测阵列检测,得到表征待测样品分子振动特征的传输谱,以此获得分子振动谱。C. The mid-infrared light source with adjustable wavelength is transformed into a parallel beam through the lens, and the graphene array structure is excited by vertical irradiation, and the detection array is used for detection to obtain the transmission spectrum that characterizes the molecular vibration characteristics of the sample to be tested, so as to obtain the molecular vibration spectrum.
进一步地,步骤A中,通过调节化学势所述的石墨烯阵列结构传输系数具有宽带的传输谱,覆盖特定待测样品在中红外频段范围内的分子振动谱,并与中红外频段分子振动形成耦合共振增强。采用石墨烯的原因是在红外和太赫兹频段,石墨烯的介电常数为负值,能够形成表面等离子谐振模,并且通过调节化学势可平滑的改变谐振频率,从而有选择性的增强场与物质的相互作用;将石墨烯带排列为阵列结构的目的是增强透射。Further, in step A, by adjusting the chemical potential, the transmission coefficient of the graphene array structure has a broadband transmission spectrum, covering the molecular vibration spectrum of the specific sample to be measured in the mid-infrared frequency range, and forming a molecular vibration spectrum with the mid-infrared frequency band. Coupling resonance enhancement. The reason for using graphene is that in the infrared and terahertz frequency bands, the dielectric constant of graphene is negative, which can form a surface plasmon resonance mode, and the resonance frequency can be smoothly changed by adjusting the chemical potential, thereby selectively enhancing the field and The interaction of matter; the purpose of arranging the graphene ribbons in an array structure is to enhance the transmission.
进一步地,步骤B2中,所述封闭的腔体不吸收电磁波,由石英等透波材料构成,起到封闭气体的作用,但不影响电磁波的透射。Further, in step B2, the closed cavity does not absorb electromagnetic waves, and is made of wave-transmissive materials such as quartz, which functions as a closed gas, but does not affect the transmission of electromagnetic waves.
本发明利用附着于石墨烯阵列结构的待测样品与局域场相互作用,引起石墨烯阵列结构宽带传输谱与待测样品分子振动谱形成耦合共振增强,从而实现分子振动谱检测,有利于发展简易、实时的分子振动谱测量仪器。The invention uses the interaction between the sample to be measured attached to the graphene array structure and the local field, causing the broadband transmission spectrum of the graphene array structure and the molecular vibration spectrum of the sample to be measured to form a coupling resonance enhancement, thereby realizing the detection of molecular vibration spectrum, which is conducive to development Simple and real-time molecular vibrational spectroscopy measurement instrument.
附图说明Description of drawings
图1为检测模型示意图;Figure 1 is a schematic diagram of the detection model;
图2为检测模型横截面;Figure 2 is a cross-section of the detection model;
图3为石墨烯介电常数与波长的关系;Fig. 3 is the relation of graphene dielectric constant and wavelength;
图4为中红外频段乙酸酐液体分子振动谱;Fig. 4 is the molecular vibration spectrum of acetic anhydride liquid in the mid-infrared frequency band;
图5为在有/无样品覆盖的情况下模拟检测阵列得到的测量结果;Figure 5 is the measurement results obtained by simulating the detection array with/without sample coverage;
图6为样品覆盖厚度对检测结果的影响。Figure 6 shows the effect of the sample coverage thickness on the test results.
具体实施方式Detailed ways
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The following will clearly and completely describe the technical solutions in the embodiments of the present invention with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only some, not all, embodiments of the present invention. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without creative efforts fall within the protection scope of the present invention.
一种基于石墨烯阵列结构的中红外分子振动谱传感方法,包括以下步骤:A kind of mid-infrared molecular vibration spectrum sensing method based on graphene array structure, comprising the following steps:
A.提供中红外频段场与物质相互作用的石墨烯阵列结构,如图1和图2所示,由石墨烯周期阵列1附着于基底介质层2上构成,被中红外平行波束垂直照射;基底材料为二氧化硅,折射率为n=1.45;石墨烯带厚度为t=1nm,宽度w=0.25μm,周期p=0.5μm;石墨烯带的介电常数为ε=1+iσ/ε0ωt,其中σ=σintra+σinter为电导率,σintra和σinter分别带间和带内的贡献;根据Kubo公式:A. The graphene array structure that provides the interaction between the mid-infrared frequency field and the substance, as shown in Figure 1 and Figure 2, is composed of a graphene periodic array 1 attached to the substrate dielectric layer 2, and is vertically irradiated by the mid-infrared parallel beam; the substrate The material is silicon dioxide, the refractive index n=1.45; the thickness of the graphene ribbon is t=1nm, the width w=0.25μm, and the period p=0.5μm; the dielectric constant of the graphene ribbon is ε=1+iσ/ε 0 ωt, where σ = σ intra + σ inter is the conductivity, and σ intra and σ inter are the contributions of the inter-band and intra-band respectively; according to the Kubo formula:
式中,T为温度,Γ载流子迁移率,μ为化学势,为普朗克常数;取温度为室温,设置T=300×kB,kB为玻尔兹曼常数,Γ=0.1meV,μ=0.3eV,得到石墨烯介电常数与频率的关系如图3所示。可以看出,在中红外3-50μm,其介电常数实部为负,而虚部(损耗)较小。where T is temperature, Γ carrier mobility, μ is chemical potential, is Planck’s constant; take temperature as room temperature, set T=300×k B , k B is Boltzmann’s constant, Γ=0.1meV, μ=0.3eV, and the relationship between graphene dielectric constant and frequency is shown in the figure 3. It can be seen that in the mid-infrared 3-50 μm, the real part of the dielectric constant is negative, while the imaginary part (loss) is small.
B1.对于液态化学物质的检测,待测样品3为乙酸酐液体,覆盖于石墨烯阵列结构上,用厚度来表示覆盖量,取厚度h=1μm,中红外频段乙酸酐分子吸收系数与频率的关系如图4所示,源于分子振动,也被称为分子振动谱;B1. For the detection of liquid chemical substances, the sample 3 to be tested is acetic anhydride liquid, which is covered on the graphene array structure, and the thickness is used to represent the covering amount. The thickness h=1 μm, the absorption coefficient of acetic anhydride molecules in the mid-infrared band and the frequency The relationship shown in Figure 4 is derived from molecular vibrations, also known as molecular vibrational spectra;
B2.对于气态化学物质的检测,将石墨烯阵列结构放置于一个封闭的腔体4中,通入待测气体,所述封闭的腔体4不吸收电磁波;B2. For the detection of gaseous chemical substances, the graphene array structure is placed in a closed cavity 4, and the gas to be measured is introduced, and the closed cavity 4 does not absorb electromagnetic waves;
C.如图2所示,用波长可调的中红外光源通过透镜5变换为平行波束,垂直照射激励石墨烯阵列结构,激励源的波长范围为8-11μm,采用检测阵列6检测,得到表征待测样品分子振动特征的传输谱,以此获得分子振动谱。C. As shown in Figure 2, use a mid-infrared light source with an adjustable wavelength to convert it into a parallel beam through the lens 5, and vertically irradiate the excitation graphene array structure. The wavelength range of the excitation source is 8-11 μm, and it is detected by the detection array 6 to obtain the characterization The transmission spectrum of the molecular vibration characteristics of the sample to be measured is used to obtain the molecular vibration spectrum.
本实施例采用时域有限差分法软件Lumerical FDTD进行了建模和仿真,在没有覆盖乙酸酐液体样品的情况下,检测阵列测量到的传输系数如图5中实线所示,可以看出,传输系数为一条近平滑的直线,覆盖了乙酸酐中红外频段分子的振动谱范围,并且其值趋近于1,表明了该结构对入射波束透明。在覆盖乙酸酐液体样品的情况下,检测阵列测量到的传输系数如图5中虚线所示,对比图4可得,传输系数的变化趋势与分子振动谱一致,达到了检测分子振动谱的目的。当待测乙酸酐样品的厚度取不同值时,检测得到的传输系数见如图6所示。可以看出,厚度越大,则传输衰减越大,越利于检测,并且由于增大厚度不影响传输系数包络的形状,因此,本发明的鲁棒性好,不易受到外界随机因素,如样品的填充厚度和不均匀性的影响。This embodiment uses the finite difference time domain method software Lumerical FDTD to carry out modeling and simulation, under the situation that does not cover acetic anhydride liquid sample, the transmission coefficient measured by the detection array is shown in the solid line in Figure 5, as can be seen, The transmission coefficient is a near-smooth straight line covering the vibrational spectrum range of acetic anhydride molecules in the mid-infrared band, and its value approaches 1, indicating that the structure is transparent to the incident beam. In the case of covering the liquid sample of acetic anhydride, the transmission coefficient measured by the detection array is shown as the dotted line in Figure 5. Compared with Figure 4, it can be seen that the change trend of the transmission coefficient is consistent with the molecular vibration spectrum, and the purpose of detecting the molecular vibration spectrum is achieved. . When the thickness of the acetic anhydride sample to be tested is different, the transmission coefficient obtained by detection is shown in Figure 6. It can be seen that the greater the thickness, the greater the transmission attenuation, which is more convenient for detection, and because increasing the thickness does not affect the shape of the envelope of the transmission coefficient, the present invention has good robustness and is less susceptible to external random factors, such as sample The effect of filling thickness and non-uniformity.
以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included in the scope of the present invention. within the scope of protection.
Claims (3)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201510053031.8A CN104568809A (en) | 2015-02-02 | 2015-02-02 | Intermediate infrared molecular vibration spectrum sensing method based on graphene array structure |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201510053031.8A CN104568809A (en) | 2015-02-02 | 2015-02-02 | Intermediate infrared molecular vibration spectrum sensing method based on graphene array structure |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN104568809A true CN104568809A (en) | 2015-04-29 |
Family
ID=53085386
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201510053031.8A Pending CN104568809A (en) | 2015-02-02 | 2015-02-02 | Intermediate infrared molecular vibration spectrum sensing method based on graphene array structure |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN104568809A (en) |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20110006837A1 (en) * | 2009-06-02 | 2011-01-13 | Feng Wang | Graphene Device, Method of Investigating Graphene, and Method of Operating Graphene Device |
| US20130193404A1 (en) * | 2012-01-26 | 2013-08-01 | Consejo Superior De Investigaciones Cientificas | Photoconversion device with enhanced photon absorption |
| CN103633183A (en) * | 2013-11-18 | 2014-03-12 | 西安电子科技大学 | Graphene medium-far infrared detector and preparing method thereof |
| CN103674880A (en) * | 2013-10-25 | 2014-03-26 | 中国科学院上海光学精密机械研究所 | TM (transverse magnetic) polarization graphene nanobelt array sensor |
| CN103776790A (en) * | 2014-02-25 | 2014-05-07 | 重庆大学 | Infrared spectrum enhancement and detection method and infrared spectrum enhancement and detection device based on graphene nano antenna |
| CN104317118A (en) * | 2014-10-24 | 2015-01-28 | 华中科技大学 | Graphene-based electric-control liquid crystal light-converging micro-lens array chip |
-
2015
- 2015-02-02 CN CN201510053031.8A patent/CN104568809A/en active Pending
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20110006837A1 (en) * | 2009-06-02 | 2011-01-13 | Feng Wang | Graphene Device, Method of Investigating Graphene, and Method of Operating Graphene Device |
| US20130193404A1 (en) * | 2012-01-26 | 2013-08-01 | Consejo Superior De Investigaciones Cientificas | Photoconversion device with enhanced photon absorption |
| CN103674880A (en) * | 2013-10-25 | 2014-03-26 | 中国科学院上海光学精密机械研究所 | TM (transverse magnetic) polarization graphene nanobelt array sensor |
| CN103633183A (en) * | 2013-11-18 | 2014-03-12 | 西安电子科技大学 | Graphene medium-far infrared detector and preparing method thereof |
| CN103776790A (en) * | 2014-02-25 | 2014-05-07 | 重庆大学 | Infrared spectrum enhancement and detection method and infrared spectrum enhancement and detection device based on graphene nano antenna |
| CN104317118A (en) * | 2014-10-24 | 2015-01-28 | 华中科技大学 | Graphene-based electric-control liquid crystal light-converging micro-lens array chip |
Non-Patent Citations (2)
| Title |
|---|
| B. VASIC´ ET AL.: "Localized surface plasmon resonances in graphene ribbon arrays for sensing of dielectric environment at infrared frequencies", 《JOURNAL OF APPLIED PHYSICS》 * |
| Y. LI ET AL.: "Graphene Plasmon Enhanced Vibrational Sensing of Surface-Adsorbed Layers", 《NANO LETTERS》 * |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Qiao et al. | Calibration-free measurement of absolute gas concentration and temperature via light-induced thermoelastic spectroscopy | |
| CN106949985B (en) | A Precise Measurement Method for Internal Temperature of Alkali Metal Gas Chamber Based on Hybrid Optical Pumping | |
| Withayachumnankul et al. | Fundamentals of measurement in terahertz time-domain spectroscopy | |
| Gao et al. | Absorbance response of a graphene oxide coated U-bent optical fiber sensor for aqueous ethanol detection | |
| US8708557B2 (en) | Apparatus for measuring thermal diffusivity | |
| CN102621083A (en) | Method and system for measuring rock optical parameters based on Terahertz time-domain spectroscopy | |
| CN104007115B (en) | Method and system for detecting jewelry structure by using terahertz time domain spectroscopic technique | |
| Meng et al. | Highly sensitive terahertz non‐destructive testing technology for stone relics deterioration prediction using SVM-based machine learning models | |
| CN107167437B (en) | An accurate measurement method of atomic density based on hybrid optical pumping | |
| CN105675536B (en) | Metal grating surface plasma bulk effect biological detection chip for THz-TDS systems | |
| JP4340814B2 (en) | Spectral analysis apparatus and spectral analysis method | |
| Junda et al. | Optical properties of soda lime float glass from 3 mm to 148 nm (0.41 meV to 8.38 eV) by spectroscopic ellipsometry | |
| CN102087211B (en) | Terahertz spectral analysis device and detection method for biofilm | |
| CN207407823U (en) | A kind of big visual field sample thickness measuring device | |
| Zhang et al. | Design and simulation of THz metasurface sensor based on transmission and reflection modes for aqueous solution detection | |
| CN111337445B (en) | Dielectric super surface based on angle scanning enhanced infrared spectrum absorption | |
| CN114563372B (en) | A method for measuring carrier concentration of terahertz band materials | |
| CN108593695A (en) | The method for directly acquiring film element component distributing from the profile data that fathoms | |
| CN104568809A (en) | Intermediate infrared molecular vibration spectrum sensing method based on graphene array structure | |
| CN112611746A (en) | Absorption spectrum detection device and detection method for material micro-area | |
| CN209485976U (en) | A special infrared transmission and reflection spectroscopy measurement accessory for slide glass sample preparation | |
| JP2012052957A (en) | Method for measuring infrared absorption spectrum | |
| Chang et al. | Surface-enhanced infrared absorption-based CO 2 sensor using photonic crystal slab | |
| CN106970033A (en) | A kind of true and false wine spectral unmixing equipment of hand-held | |
| Hinrichs et al. | Field manipulation of infrared absorption properties in thin films |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| WD01 | Invention patent application deemed withdrawn after publication | ||
| WD01 | Invention patent application deemed withdrawn after publication |
Application publication date: 20150429 |