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TWI407092B - Raman scattering substrate and detection system having the same - Google Patents

Raman scattering substrate and detection system having the same Download PDF

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TWI407092B
TWI407092B TW98132197A TW98132197A TWI407092B TW I407092 B TWI407092 B TW I407092B TW 98132197 A TW98132197 A TW 98132197A TW 98132197 A TW98132197 A TW 98132197A TW I407092 B TWI407092 B TW I407092B
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carbon nanotube
raman scattering
scattering substrate
metal particles
film
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TW98132197A
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TW201111771A (en
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ying-hui Sun
Kai Liu
Kai-Li Jiang
Jiao Miao
Shou-Shan Fan
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Hon Hai Prec Ind Co Ltd
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Abstract

The invention relates to a raman scattering substrate. The raman scattering substrate includes a carbon nanotube composite film. The carbon nanotube composite film includes at least one carbon nanotube film and a plurality of metal partials. The carbon nanotube film includes a plurality of carbon nanotubes. The metal partials are disposed on the surface of the carbon nanotubes. The invention also relates a raman detecting system including the raman scattering substrate.

Description

拉曼散射基底及具該拉曼散射基底之檢測系統 Raman scattering substrate and detection system having the same

本發明涉及一種拉曼散射基底及具該拉曼散射基底之檢測系統。 The present invention relates to a Raman scattering substrate and a detection system having the same.

印度物理學家拉曼(C.V.Raman)於1928年首先發現了單色光於透過四氯化碳液體之後散射光之頻率發生變化之現象,之後,人們將這種現象稱之為拉曼效應,產生頻率變化後之散射光為拉曼光譜。拉曼光譜能夠獲得分子或官能團振動模式之資訊,稱之為分子之“指紋光譜”,其可提供分子之詳細結構資訊,如化學鍵之類型、強度、角度、構像變化等。然普通之拉曼散射訊號強度很低,難以對樣品分子直接進行探測,直到Fleischman等人於1974年於銀電極粗糙表面吸附吡啶得到吡啶增強之拉曼散射訊號。表面增強拉曼散射(Surface-enhanced Raman Scattering,SERS)效應係指吸附於拉曼散射基底如銀電極粗糙表面之分子其拉曼散射訊號增強之現象。表面增強拉曼散射可用來研究表面吸附分子種類、確定分子於表面之取向和表面反應之有利工具。 In 1928, the Indian physicist CVRaman first discovered the phenomenon that the frequency of scattered light transmitted by monochromatic light after passing through a carbon tetrachloride liquid. Later, this phenomenon was called the Raman effect. The scattered light after the frequency change is generated is a Raman spectrum. Raman spectroscopy can obtain information about the vibration mode of a molecule or a functional group, called a "fingerprint spectrum" of a molecule, which provides detailed structural information of the molecule, such as the type, strength, angle, and conformational change of the chemical bond. However, the ordinary Raman scattering signal has low intensity, and it is difficult to directly detect the sample molecules until Fleischman et al. adsorbed pyridine on the rough surface of the silver electrode in 1974 to obtain a pyridine-enhanced Raman scattering signal. The Surface-enhanced Raman Scattering (SERS) effect refers to the phenomenon that the Raman scattering signal is enhanced by molecules adsorbed on the rough surface of a Raman scattering substrate such as a silver electrode. Surface-enhanced Raman scattering can be used to study the surface adsorption of molecular species, the identification of molecules on the surface orientation and surface reactions.

製備穩定、高增強因數之拉曼散射基底係研究表面增強拉曼 散射效應之重要基礎。傳統拉曼散射基底主要係通過於一平面基底表面形成複數金屬顆粒而形成,在該平面基底形成金屬顆粒之方法包括電化學、蒸鍍、濺鍍等。如杜一平等人於2008年6月5日申請,並於2008年10月29日公開之中國大陸第CN101294904A號專利申請,介紹了一種拉曼散射基底之製備方法,該方法通過電化學方法製備銀溶膠並將該銀溶膠設置於一基底形成以拉曼散射基底。利用該方法製備之拉曼散射基底,由於金屬顆粒容易聚集而難以使該金屬顆粒做到密集排佈,從而難以得到高靈敏性之拉曼散射基底。 Preparation of stable, high enhancement factor Raman scattering substrate system for surface enhanced Raman An important basis for the scattering effect. Conventional Raman scattering substrates are mainly formed by forming a plurality of metal particles on the surface of a planar substrate, and methods for forming metal particles on the planar substrate include electrochemistry, evaporation, sputtering, and the like. A method for preparing a Raman scattering substrate, which is prepared by an electrochemical method, is described in Chinese Patent Application No. CN101294904A, which is filed on Jun. 5, 2008, and issued on October 29, 2008. The silver sol is disposed on a substrate to form a Raman scattering substrate. The Raman scattering substrate prepared by this method is difficult to make the metal particles densely arranged due to the easy aggregation of the metal particles, so that it is difficult to obtain a highly sensitive Raman scattering substrate.

有鑒於此,提供一種其金屬顆粒能夠密集排佈之拉曼散射基底及具該拉曼散射基底之檢測系統實為必要。 In view of the above, it is necessary to provide a Raman scattering substrate in which metal particles can be densely arranged and a detection system having the Raman scattering substrate.

一種拉曼散射基底,其包括一奈米碳管複合膜。該奈米碳管複合膜包括至少一奈米碳管膜及複數金屬顆粒。該奈米碳管膜包括複數均勻分佈之奈米碳管,該複數金屬顆粒設置於該複數奈米碳管表面。 A Raman scattering substrate comprising a carbon nanotube composite membrane. The carbon nanotube composite membrane comprises at least one carbon nanotube membrane and a plurality of metal particles. The carbon nanotube film comprises a plurality of uniformly distributed carbon nanotubes, and the plurality of metal particles are disposed on the surface of the plurality of carbon nanotubes.

一種拉曼散射基底,其包括一奈米碳管複合膜。該奈米碳管複合膜包括由兩層奈米碳管膜層疊交叉設置形成之一膜狀結構。一緩衝層設置於該膜狀結構表面,複數金屬顆粒設置於該緩衝層背向該膜狀結構之表面。該奈米碳管膜包括複數奈米碳管相互大致平行且大致平行於該奈米碳管膜表面。 A Raman scattering substrate comprising a carbon nanotube composite membrane. The carbon nanotube composite membrane comprises a film-like structure formed by laminating two layers of carbon nanotube membranes. A buffer layer is disposed on the surface of the film structure, and the plurality of metal particles are disposed on the surface of the buffer layer facing away from the film structure. The carbon nanotube membrane includes a plurality of carbon nanotubes that are substantially parallel to each other and substantially parallel to the surface of the carbon nanotube membrane.

一種拉曼檢測系統,其包括一發射模塊、一拉曼散射基底及一接收模塊。該發射模塊用於向該拉曼散射基底發射一光束 。該拉曼散射基底用於將該發射模塊發射過來之光束進行散射。該接收模塊用於收集從該拉曼散射基底散射之散射光,形成一拉曼光譜特徵圖。該拉曼散射基底包括一奈米碳管複合膜。該奈米碳管複合膜包括至少一奈米碳管膜及複數金屬顆粒。該奈米碳管膜包括複數均勻分佈之奈米碳管,該複數金屬顆粒設置於該複數奈米碳管表面。 A Raman detection system includes a transmitting module, a Raman scattering substrate, and a receiving module. The transmitting module is configured to emit a light beam to the Raman scattering substrate . The Raman scattering substrate is used to scatter the light beam emitted by the transmitting module. The receiving module is configured to collect scattered light scattered from the Raman scattering substrate to form a Raman spectral feature map. The Raman scattering substrate comprises a carbon nanotube composite membrane. The carbon nanotube composite membrane comprises at least one carbon nanotube membrane and a plurality of metal particles. The carbon nanotube film comprises a plurality of uniformly distributed carbon nanotubes, and the plurality of metal particles are disposed on the surface of the plurality of carbon nanotubes.

相較於先前技術,該拉曼散射基底包括一奈米碳管複合膜,該奈米碳管複合膜包括複數具有較小尺寸和較大比表面積之奈米碳管。因此,該金屬能夠以較小之粒徑密集排佈於該奈米碳管複合膜表面。從而使該拉曼散射基底具有較好之穩定性與靈敏性。 Compared to the prior art, the Raman scattering substrate comprises a carbon nanotube composite membrane comprising a plurality of carbon nanotubes having a smaller size and a larger specific surface area. Therefore, the metal can be densely arranged on the surface of the carbon nanotube composite film with a small particle diameter. Thereby, the Raman scattering substrate has better stability and sensitivity.

100、200、300‧‧‧檢測系統 100, 200, 300‧‧‧ inspection systems

110、210、310‧‧‧發射模塊 110, 210, 310‧‧‧ launch module

120、220、320‧‧‧拉曼散射基底 120, 220, 320‧‧‧ Raman scattering substrate

121‧‧‧支撐結構 121‧‧‧Support structure

122、222、322‧‧‧奈米碳管複合膜 122, 222, 322‧‧‧ nano carbon tube composite film

130、230、330‧‧‧接收模塊 130, 230, 330‧‧‧ receiving modules

221‧‧‧框架 221‧‧‧Frame

321‧‧‧基底 321‧‧‧Base

圖1係本發明第一實施例應用一拉曼散射基底之檢測系統之結構示意圖。 1 is a schematic view showing the structure of a detection system using a Raman scattering substrate according to a first embodiment of the present invention.

圖2係圖1中拉曼散射基底中之奈米碳管絮化膜之掃描電鏡照片。 2 is a scanning electron micrograph of a carbon nanotube flocculation film in the Raman scattering substrate of FIG.

圖3係圖1中拉曼散射基底中之奈米碳管碾壓膜之掃描電鏡照片。 3 is a scanning electron micrograph of a carbon nanotube rolled film in the Raman scattering substrate of FIG.

圖4係圖1中拉曼散射基底中之奈米碳管拉膜之掃描電鏡照片。 Figure 4 is a scanning electron micrograph of the carbon nanotube film in the Raman scattering substrate of Figure 1.

圖5係圖1中拉曼散射基底中之奈米碳管複合膜之透射電鏡照片。 Figure 5 is a transmission electron micrograph of the carbon nanotube composite membrane in the Raman scattering substrate of Figure 1.

圖6係圖1中拉曼散射基底中由奈米碳管、金屬顆粒形成之奈米碳管複合膜與由奈米碳管形成之奈米碳管膜檢測待測樣品為2.5×10-3摩爾每升之吡啶水溶液時所得到之拉曼光譜特性圖。 6 is a carbon nanotube composite film formed by a carbon nanotube and a metal particle in a Raman scattering substrate of FIG. 1 and a carbon nanotube film formed by a carbon nanotube film; the sample to be tested is 2.5×10 −3 mol per Raman spectral characteristics obtained when the aqueous solution of pyridine is ascended.

圖7係圖1中拉曼散射基底中由奈米碳管、金屬顆粒形成之奈米碳管複合膜與由奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。 Figure 7 is a diagram showing the carbon nanotube film formed by carbon nanotubes and metal particles in the Raman scattering substrate of Figure 1 and the carbon nanotube film formed by the carbon nanotubes. The sample to be tested is 10 -6 moles per liter. Raman spectral characteristics obtained when rhodamine ethanol solution.

圖8係本發明第二實施例應用一拉曼散射基底之檢測系統之結構示意圖。 Figure 8 is a block diagram showing the structure of a detection system using a Raman scattering substrate in accordance with a second embodiment of the present invention.

圖9係圖8中拉曼散射基底中之奈米碳管複合膜之透射電鏡照片。 Figure 9 is a transmission electron micrograph of the carbon nanotube composite membrane in the Raman scattering substrate of Figure 8.

圖10係圖8中拉曼散射基底中由奈米碳管、緩衝層、金屬顆粒形成之奈米碳管複合膜與由奈米碳管形成之奈米碳管膜檢測待測樣品為2.5×10-3摩爾每升之吡啶水溶液時所得到之拉曼光譜特性圖。 10 is a carbon nanotube composite film formed by a carbon nanotube, a buffer layer, and a metal particle in a Raman scattering substrate of FIG. 8 and a carbon nanotube film formed by a carbon nanotube film. The sample to be tested is 2.5×10 Raman spectral characteristics obtained when 3 moles of pyridine aqueous solution per liter.

圖11係圖8中拉曼散射基底中由奈米碳管、緩衝層、金屬顆粒形成之奈米碳管複合膜與由奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。 11 is a 10-20 m mole of a sample of a carbon nanotube composite film formed by a carbon nanotube, a buffer layer, and a metal particle in a Raman scattering substrate of FIG. 8 and a carbon nanotube film formed by a carbon nanotube. Raman spectral characteristics obtained per liter of rhodamine ethanol solution.

圖12係圖8中拉曼散射基底中由奈米碳管、緩衝層與金屬顆粒形成之奈米碳管複合膜、圖1中由奈米碳管、緩衝層與金 屬顆粒形成之奈米碳管複合膜及由奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。 12 is a composite of a carbon nanotube composite film formed of a carbon nanotube, a buffer layer and a metal particle in the Raman scattering substrate of FIG. 8, and a carbon nanotube formed by a carbon nanotube, a buffer layer and a metal particle in FIG. The film and the carbon nanotube film formed by the carbon nanotubes are used to detect a Raman spectral characteristic map obtained when the sample to be tested is 10 -6 moles per liter of rhodamine ethanol solution.

圖13係本發明第三實施例應用一拉曼散射基底之檢測系統之結構示意圖。 Figure 13 is a block diagram showing the structure of a detection system using a Raman scattering substrate in accordance with a third embodiment of the present invention.

圖14係圖13中拉曼散射基底部分放大結構示意圖。 Figure 14 is a schematic enlarged view showing a portion of the Raman scattering substrate of Figure 13.

圖15係圖13中拉曼散射基底中由多壁奈米碳管、金屬顆粒形成之奈米碳管複合膜與由多壁奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。 15 is a view showing a sample of a carbon nanotube film formed by a multi-walled carbon nanotube and a metal particle in a Raman scattering substrate of FIG. 13 and a carbon nanotube film formed by a multi-walled carbon nanotube; Raman spectral characteristics obtained when -6 moles per liter of rhodamine ethanol solution.

圖16係圖13中拉曼散射基底中由單壁奈米碳管、13奈米~17奈米金屬顆粒形成之奈米碳管複合膜、圖13中拉曼散射基底中由單壁奈米碳管、28奈米~32奈米金屬顆粒形成之奈米碳管複合膜及由單壁奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。 Figure 16 is a diagram showing a nano-carbon nanotube composite film formed of a single-walled carbon nanotube, a 13 nm to 17 nm metal particle in the Raman scattering substrate of Fig. 13, and a single-walled nanoparticle in the Raman scattering substrate of Fig. 13. The carbon nanotubes, the nanocarbon tube composite film formed by 28 nm to 32 nm metal particles, and the carbon nanotube film formed by the single-walled carbon nanotubes are 10 to 6 moles per liter of rhodamine. Raman spectral characteristics obtained in ethanol solution.

以下將結合附圖對本發明作進一步詳細之說明。 The invention will be further described in detail below with reference to the accompanying drawings.

一種檢測系統100,其包括一發射模塊110、一拉曼散射基底120及一接收模塊130。 A detection system 100 includes a transmitting module 110, a Raman scattering substrate 120, and a receiving module 130.

該發射模塊110用於向該拉曼散射基底120發射一光束,以便於該拉曼散射基底120形成散射光。具體地,該光束照射於 該拉曼散射基底120表面之光斑面積小於2平方微米。該光束為頻寬較小且具有固定頻率之強光源,如氬離子鐳射。優選地,該光束之波長於450.0奈米~514.5奈米之間。在本實施例中,該光束之波長為514.5奈米之綠光,514.5奈米之綠光相對其他波長之光於相同功率下具有較大之散射光強。 The transmitting module 110 is configured to emit a light beam to the Raman scattering substrate 120 to facilitate the Raman scattering substrate 120 to form scattered light. Specifically, the light beam is irradiated The spot area of the surface of the Raman scattering substrate 120 is less than 2 square microns. The beam is a strong source with a small bandwidth and a fixed frequency, such as an argon ion laser. Preferably, the wavelength of the beam is between 450.0 nm and 514.5 nm. In this embodiment, the wavelength of the light beam is 514.5 nanometers of green light, and the green light of 514.5 nanometers has a larger scattered light intensity at the same power than the light of other wavelengths.

該拉曼散射基底120用於承載一待測樣品,並將該發射模塊110發射過來之光束進行散射,形成具有待測樣品分子結構資訊之散射光。當該光束發射於該拉曼散射基底120時,該光束將照射到被該拉曼散射基底120吸附之待測樣品分子,該光束中之光子與待測樣品分子碰撞。光子與待測樣品分子碰撞,發生動量改變,從而改變光子之方向,向四方散射;部分光子於碰撞時還與待測樣品分子發生能量交換,改變光子之能量或頻率,使該光子具有待測樣品分子結構資訊。即該光束與吸附於該拉曼散射基底120之待測樣品分子發生碰撞後,將形成具有該待測樣品分子結構資訊之散射光。該待測樣品可為固態樣品(如樣品粉末、吸附有樣品之固體顆粒等)及液態樣品(如內溶樣品成分之液滴、熔融態樣品等)。在檢測時,該待測樣品與該拉曼散射基底120直接接觸。 The Raman scattering substrate 120 is configured to carry a sample to be tested, and scatter the light beam emitted by the transmitting module 110 to form scattered light having information about the molecular structure of the sample to be tested. When the light beam is emitted on the Raman scattering substrate 120, the light beam will be irradiated to the sample molecules to be tested adsorbed by the Raman scattering substrate 120, and the photons in the light beam collide with the sample molecules to be tested. The photons collide with the molecules of the sample to be tested, and the momentum changes, thereby changing the direction of the photons and scattering to the square. When some photons collide, they also exchange energy with the molecules of the sample to be tested, changing the energy or frequency of the photons, so that the photons have to be tested. Sample molecular structure information. That is, after the beam collides with the sample molecule to be tested adsorbed on the Raman scattering substrate 120, scattered light having information about the molecular structure of the sample to be tested is formed. The sample to be tested may be a solid sample (such as a sample powder, a solid particle to which a sample is adsorbed, etc.) and a liquid sample (such as a droplet of an internally dissolved sample component, a molten sample, etc.). The sample to be tested is in direct contact with the Raman scattering substrate 120 at the time of detection.

該拉曼散射基底120包括一支撐結構121及一奈米碳管複合膜122。 The Raman scattering substrate 120 includes a support structure 121 and a carbon nanotube composite film 122.

該支撐結構121用於固定或支撐該奈米碳管複合膜122。具體地,該支撐結構121可選用玻璃基底、透明塑膠基底、柵網或框架。當該支撐結構121為柵網或框架時,該奈米碳管複 合膜122可通過該支撐結構121至少部分懸空設置,此時該奈米碳管複合膜122之懸空面積應大於2平方微米,即大於該光束之光斑面積,該光束照射至該奈米碳管複合膜122之懸空部分。當該支撐結構121為玻璃基底或透明塑膠基底時,該奈米碳管複合膜122貼合於該支撐結構121之表面,此時,該支撐結構121應具有較好之透光率。在本實施例中,該支撐結構121為一框架,該框架固定於該奈米碳管複合膜122四週以固定該奈米碳管複合膜122,並使奈米碳管複合膜122懸空設置。使該奈米碳管複合膜122至少部分懸空設置或者設置於一透射率較高之支撐結構121表面,儘量使照射於該奈米碳管複合膜122中之光束中沒有被散射之光子能夠透過,以免這部分光子經過反射後再照射到奈米碳管複合膜122中之奈米碳管上產生散射光,該散射光會對具待測樣品分子結構資訊之散射光干擾。從而不利於該拉曼檢測系統100對待測樣品之檢測。 The support structure 121 is used to fix or support the carbon nanotube composite film 122. Specifically, the support structure 121 may be a glass substrate, a transparent plastic substrate, a grid or a frame. When the support structure 121 is a grid or a frame, the carbon nanotubes are complex The film 122 can be at least partially suspended by the support structure 121. At this time, the suspended area of the carbon nanotube composite film 122 should be greater than 2 square micrometers, that is, larger than the spot area of the light beam, and the light beam is irradiated to the carbon nanotube. The suspended portion of the composite film 122. When the support structure 121 is a glass substrate or a transparent plastic substrate, the carbon nanotube composite film 122 is attached to the surface of the support structure 121. At this time, the support structure 121 should have a good light transmittance. In this embodiment, the support structure 121 is a frame, and the frame is fixed around the carbon nanotube composite film 122 to fix the carbon nanotube composite film 122, and the carbon nanotube composite film 122 is suspended. The carbon nanotube composite film 122 is at least partially suspended or disposed on a surface of the support structure 121 having a high transmittance, and the photons that are not scattered by the light beam irradiated into the carbon nanotube composite film 122 are transmitted as far as possible. In order to prevent this part of the photons from being reflected and then irradiated onto the carbon nanotubes in the carbon nanotube composite film 122, scattered light is generated, which will interfere with the scattered light of the molecular structure information of the sample to be tested. This is not conducive to the detection of the sample to be tested by the Raman detection system 100.

該奈米碳管複合膜122包括至少一奈米碳管膜及設置於該奈米碳管膜表面之複數金屬顆粒,該奈米碳管膜包括複數均勻分佈之奈米碳管。優選地,每一奈米碳管表面均設置有至少一金屬顆粒。在本實施例中,該奈米碳管膜為一自支撐結構,所謂“自支撐”即該奈米碳管膜無需通過設置於一基體表面,也能保持自身特定之形狀。 The carbon nanotube composite membrane 122 includes at least one carbon nanotube membrane and a plurality of metal particles disposed on the surface of the carbon nanotube membrane, the carbon nanotube membrane comprising a plurality of uniformly distributed carbon nanotubes. Preferably, at least one metal particle is disposed on the surface of each carbon nanotube. In this embodiment, the carbon nanotube film is a self-supporting structure, and the so-called "self-supporting" means that the carbon nanotube film can maintain its own specific shape without being disposed on a surface of a substrate.

請參閱圖2,該奈米碳管膜可為由該複數奈米碳管相互纏繞而形成之奈米碳管絮化膜,該絮化膜各向同性。該奈米碳管 絮化膜之厚度於0.5奈米~100微米之間且具有複數孔徑於1奈米~500奈米之間之間隙。該奈米碳管絮化膜中,相互纏繞之奈米碳管通過凡德瓦爾力相互吸引,從而形成一自支撐之奈米碳管膜。 Referring to FIG. 2, the carbon nanotube film may be a carbon nanotube flocculation film formed by intertwining the plurality of carbon nanotubes, and the flocculation film is isotropic. The carbon nanotube The thickness of the flocculated membrane is between 0.5 nm and 100 μm and has a complex pore diameter of between 1 nm and 500 nm. In the carbon nanotube flocculation film, the intertwined carbon nanotubes are attracted to each other by van der Waals force to form a self-supporting carbon nanotube film.

該奈米碳管膜還可為由該複數奈米碳管沿一個方向或複數方向擇優取向排列而形成之奈米碳管碾壓膜,相鄰之奈米碳管由凡德瓦爾力結合。該奈米碳管碾壓膜之厚度於0.5奈米~100微米之間且相鄰奈米碳管之間之間隙於1奈米~500奈米之間。該奈米碳管碾壓膜可採用一平面壓頭沿垂直於上述奈米碳管陣列生長之基底之方向擠壓上述奈米碳管陣列而獲得,此時該奈米碳管碾壓膜中之奈米碳管各向同性;請參閱圖3,該奈米碳管碾壓膜也可採用一滾軸狀壓頭沿某一固定方向碾壓上述奈米碳管陣列而獲得,此時該奈米碳管碾壓膜中之奈米碳管於該固定方向擇優取向;該奈米碳管碾壓膜還可採用滾軸狀壓頭沿不同方向碾壓上述奈米碳管陣列而獲得,此時該奈米碳管碾壓膜中之奈米碳管沿不同方向擇優取向。 The carbon nanotube film may also be a carbon nanotube rolled film formed by arranging the plurality of carbon nanotubes in a preferred orientation in one direction or in a plurality of directions, and the adjacent carbon nanotubes are combined by van der Waals force. The thickness of the carbon nanotube rolled film is between 0.5 nm and 100 μm and the gap between adjacent carbon nanotubes is between 1 nm and 500 nm. The carbon nanotube rolled film can be obtained by extruding the carbon nanotube array in a direction perpendicular to the substrate grown by the carbon nanotube array in a planar indenter, and the carbon nanotube is laminated in the film. The carbon nanotube is isotropic; referring to FIG. 3, the carbon nanotube rolled film can also be obtained by rolling the carbon nanotube array in a fixed direction by a roller-shaped indenter. The carbon nanotubes in the carbon nanotube rolled film are preferentially oriented in the fixed direction; the carbon nanotube rolled film can also be obtained by rolling the above-mentioned carbon nanotube array in different directions by a roller-shaped indenter. At this time, the carbon nanotubes in the carbon nanotube rolled film are preferentially oriented in different directions.

請參閱圖4,該奈米碳管膜還可為由該複數奈米碳管大致相互平行且大致平行於該奈米碳管膜表面而形成之奈米碳管拉膜,進一步地,該複數奈米碳管通過凡德瓦爾力相互吸引並首尾相連且沿同一方向擇優取向排列。該奈米碳管拉膜為一自支撐之奈米碳管膜,為從一奈米碳管陣列中拉取而獲得。該奈米碳管拉膜之厚度於0.5奈米~100微米之間且相鄰奈米碳管之間之間隙於1奈米~500奈米之間。 Referring to FIG. 4, the carbon nanotube film may further be a carbon nanotube film formed by the plurality of carbon nanotubes being substantially parallel to each other and substantially parallel to the surface of the carbon nanotube film. Further, the plurality The carbon nanotubes are attracted to each other by Van der Waals forces and are connected end to end and arranged in the same direction. The carbon nanotube film is a self-supporting carbon nanotube film obtained by pulling from a carbon nanotube array. The thickness of the carbon nanotube film is between 0.5 nm and 100 μm and the gap between adjacent carbon nanotubes is between 1 nm and 500 nm.

當該奈米碳管複合膜122包括複數奈米碳管拉膜時,該複數奈米碳管拉膜層疊設置形成一層狀結構。該層狀結構之厚度不限,相鄰之奈米碳管拉膜通過凡德瓦爾力結合。優選地,該層狀結構包括之奈米碳管膜之層數小於或等於10層,從而使單位面積內之奈米碳管數量較少,使該奈米碳管自身之拉曼光強保持於較小之範圍,從而減小拉曼光譜中奈米碳管之拉曼峰強。該層狀結構中相鄰之奈米碳管拉膜中之奈米碳管之間具有一交叉角度α,且該α大於0度且小於等於90度。當相鄰之奈米碳管拉膜中之奈米碳管之間具有一交叉角度α時,該複數奈米碳管拉膜中之奈米碳管相互交織形成一網狀結構,使該奈米碳管複合膜122之機械性能增加,同時使該奈米碳管複合膜122具有複數均勻且規則排佈之微孔,該微孔孔徑於1奈米~500奈米之間。可以理解,當該拉曼散射基底100承載之待測樣品為溶液時,該網狀結構容易使滴於該奈米碳管拉膜表面之溶液液滴形成一均勻分散之溶液膜,從而方便檢測。同時形成該網狀結構之奈米碳管相互搭接之“節點”對樣品之吸附性較好,能夠提高該奈米碳管複合膜122對樣品之靈敏度。在本實施例中,該奈米碳管複合膜122包括兩層奈米碳管拉膜層疊設置,相鄰之奈米碳管膜中之奈米碳管之間之交叉角度α大致等於90度,形成一網狀結構。 When the carbon nanotube composite film 122 includes a plurality of carbon nanotube film, the plurality of carbon nanotube films are laminated to form a layered structure. The thickness of the layered structure is not limited, and the adjacent carbon nanotube film is bonded by van der Waals force. Preferably, the layered structure comprises a layer of carbon nanotube film of less than or equal to 10 layers, so that the number of carbon nanotubes per unit area is small, so that the Raman light intensity of the carbon nanotube itself is maintained. In a smaller range, the Raman peak intensity of the carbon nanotubes in the Raman spectrum is reduced. The carbon nanotubes in the adjacent carbon nanotube film in the layered structure have an intersection angle α between the α and the α is greater than 0 degrees and less than or equal to 90 degrees. When the carbon nanotubes in the adjacent carbon nanotube film have an intersection angle α, the carbon nanotubes in the composite carbon nanotube film are interwoven to form a network structure, so that the nanosphere is The mechanical properties of the carbon nanotube composite membrane 122 are increased, and the carbon nanotube composite membrane 122 has a plurality of uniform and regularly arranged micropores having a pore diameter of between 1 nm and 500 nm. It can be understood that when the sample to be tested carried by the Raman scattering substrate 100 is a solution, the network structure easily forms a solution film of the solution dripping on the surface of the carbon nanotube film to form a uniformly dispersed solution film, thereby facilitating detection. . At the same time, the "node" of the carbon nanotubes forming the network structure overlaps with each other, and the sensitivity of the carbon nanotube composite film 122 to the sample can be improved. In this embodiment, the carbon nanotube composite film 122 comprises two layers of carbon nanotube film laminated, and the intersection angle α between the carbon nanotubes in the adjacent carbon nanotube film is approximately equal to 90 degrees. Forming a network structure.

該金屬顆粒可通過將一金屬材料用電子束蒸鍍法或電子束濺鍍法形成於該奈米碳管表面。具體地,當通過電子束蒸鍍或電子束濺鍍法形成之金屬氣體接觸到奈米碳管之管壁時,該 金屬氣體會於奈米碳管之管壁表面沈積。由於金屬之表面張力之作用,其會於奈米碳管表面聚集成金屬顆粒。優選地,該金屬顆粒通過電子束蒸鍍法形成於每一奈米碳管表面,同一奈米碳管表面形成有複數相互間隔之金屬顆粒。該金屬顆粒之形成及粒徑之大小可通過控制奈米碳管表面金屬材料之蒸鍍量來控制,該蒸鍍量不能過大,以免過多之金屬材料沈積於該奈米碳管表面,形成一金屬膜而非金屬顆粒。可以理解,在實際蒸鍍過程中,需要通過監測金屬材料之厚度來控制奈米碳管表面金屬材料之蒸鍍量。具體地,該金屬材料於奈米碳管膜表面之厚度應控制於1奈米~100奈米之間,使其以金屬顆粒之形式存在。該金屬顆粒之材料包括過渡金屬或貴金屬,優選地,該金屬顆粒之材料包括金、銀、銅及鈀中之一種或多種;該金屬顆粒為准球形,其粒徑於1奈米~100奈米之間,優選地,其粒徑於18奈米~22奈米之間;相鄰兩個金屬顆粒之間之間隙於1奈米~15奈米之間,優選地,相鄰兩個金屬顆粒之間之間隙於1奈米~5奈米之間。可以理解,由於該金屬顆粒之粒徑較小且相鄰金屬顆粒之間隔較小,同時該金屬顆粒之粒徑及相鄰金屬顆粒之間之間隔均比較均勻。在外界入射光電磁場激發下,金屬表面等離子發生共振吸收,使得顆粒間局域電磁場增強,從而導致分子之拉曼訊號增強從而提升該拉曼散射基底120之靈敏度。 The metal particles may be formed on the surface of the carbon nanotube by electron beam evaporation or electron beam sputtering. Specifically, when the metal gas formed by electron beam evaporation or electron beam sputtering is in contact with the wall of the carbon nanotube, The metal gas is deposited on the surface of the tube wall of the carbon nanotube. Due to the surface tension of the metal, it will aggregate into metal particles on the surface of the carbon nanotube. Preferably, the metal particles are formed on the surface of each of the carbon nanotubes by electron beam evaporation, and a plurality of metal particles spaced apart from each other are formed on the surface of the same carbon nanotube. The formation of the metal particles and the size of the particle diameter can be controlled by controlling the evaporation amount of the metal material on the surface of the carbon nanotube. The evaporation amount should not be too large, so as to prevent excessive metal material from depositing on the surface of the carbon nanotube to form a Metal film instead of metal particles. It can be understood that in the actual evaporation process, it is necessary to control the evaporation amount of the metal material on the surface of the carbon nanotube by monitoring the thickness of the metal material. Specifically, the thickness of the metal material on the surface of the carbon nanotube film should be controlled between 1 nm and 100 nm, so that it exists in the form of metal particles. The material of the metal particles comprises a transition metal or a noble metal. Preferably, the material of the metal particles comprises one or more of gold, silver, copper and palladium; the metal particles are quasi-spherical and have a particle diameter of from 1 nm to 100 nm. Between meters, preferably, the particle size is between 18 nm and 22 nm; the gap between two adjacent metal particles is between 1 nm and 15 nm, preferably, two adjacent metals The gap between the particles is between 1 nm and 5 nm. It can be understood that since the particle diameter of the metal particles is small and the interval between adjacent metal particles is small, the particle diameter of the metal particles and the interval between adjacent metal particles are relatively uniform. Under the excitation of the external incident photoelectric magnetic field, the metal surface plasma resonates and absorbs, so that the local electromagnetic field between the particles is enhanced, thereby causing the Raman signal enhancement of the molecule to enhance the sensitivity of the Raman scattering substrate 120.

請參照圖5,為本實施例奈米碳管複合膜122之透射電鏡照片,該奈米碳管複合膜122中之複數奈米碳管形成有兩個層疊 且交叉設置之奈米碳管膜。該複數奈米碳管外表面間隔設置有多晶結構之銀顆粒,該銀顆粒之粒徑於18奈米~22奈米之間;相鄰兩個銀顆粒之間之間隙於1奈米~5奈米之間。 Referring to FIG. 5, a transmission electron micrograph of the carbon nanotube composite film 122 of the present embodiment, the plurality of carbon nanotubes in the carbon nanotube composite film 122 are formed into two layers. And set the carbon nanotube film. The outer surface of the plurality of carbon nanotubes is spaced apart by a silver particle having a polycrystalline structure, and the particle size of the silver particle is between 18 nm and 22 nm; the gap between two adjacent silver particles is 1 nm~ Between 5 nanometers.

該拉曼散射基底120接收到該發射模塊110發射過來之光束時,該拉曼散射基底120中之複數金屬顆粒形成一漫反射面,對該光束進行漫反射。當該金屬顆粒表面吸附有待測樣品時,照射於該金屬顆粒表面之光束與該待測樣品中之分子或官能團發生彈性碰撞或非彈性碰撞。發生非彈性碰撞之光子能量發生改變,並具有該待測分子之結構資訊,形成頻率變化之散射光。具體地,該結構資訊為每個分子或官能團之振動模式,該振動模式為該分子之獨特特徵。 When the Raman scattering substrate 120 receives the light beam emitted by the emitting module 110, the plurality of metal particles in the Raman scattering substrate 120 form a diffuse reflecting surface, and the light beam is diffusely reflected. When the sample to be tested is adsorbed on the surface of the metal particle, the light beam irradiated on the surface of the metal particle elastically collides or inelastically collides with the molecule or functional group in the sample to be tested. The photon energy of the inelastic collision changes, and has the structural information of the molecule to be tested, forming a scattered light with a frequency change. Specifically, the structural information is a vibration mode of each molecule or functional group, which is a unique feature of the molecule.

該接收模塊130用於收集從該拉曼散射基底120散射之散射光,形成一拉曼光譜特徵圖。具體地,該接收模塊130可為多通道光子檢測器如電子耦合器件,也可為單通道光子檢測器如光電倍增管。從該拉曼光譜特性圖可讀出該待測樣品分子或官能團之振動模式及其對應之分子或官能團。 The receiving module 130 is configured to collect scattered light scattered from the Raman scattering substrate 120 to form a Raman spectral feature map. Specifically, the receiving module 130 can be a multi-channel photon detector such as an electronic coupling device, or a single-channel photon detector such as a photomultiplier tube. From the Raman spectral property map, the vibration mode of the molecule or functional group of the sample to be tested and its corresponding molecule or functional group can be read.

該待測樣品包括固態樣品(如樣品粉末、吸附有樣品之固體顆粒等)及液態樣品(如內溶樣品成分之液滴、熔融態樣品等)。在本實施例中,該待測樣品分別選擇2.5×10-3摩爾每升之吡啶水溶液及濃度為10-6摩爾每升之若丹明乙醇溶液。該待測樣品吸附於該拉曼散射基底120中之金屬顆粒表面。請參閱圖6,圖6為本實施例中檢測系統100中由奈米碳管、金屬顆粒形成之奈米碳管複合膜122與由奈米碳管形成之奈 米碳管膜檢測待測樣品為2.5×10-3摩爾每升之吡啶水溶液時所得到之拉曼光譜特性圖。從圖中可看出,該吡啶之拉曼散射峰強於該檢測系統100中得到了顯著增強,可清晰地分辯該吡啶之各個化學鍵之振動模式。請參閱圖7,圖7為本實施例中檢測系統100中由奈米碳管、金屬顆粒形成之奈米碳管複合膜122及與奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。從圖中可看出,儘管該羅丹明之分子為螢光分子,通常螢光分子之拉曼訊號都被螢光背景掩蓋,然而在該檢測系統100中其拉曼散射峰強於可得到顯著增強。 The sample to be tested includes a solid sample (such as a sample powder, solid particles adsorbed with the sample, etc.) and a liquid sample (such as a droplet of an internally dissolved sample component, a molten sample, etc.). In the present embodiment, the sample to be tested is selected from 2.5 × 10 -3 moles per liter of pyridine aqueous solution and a concentration of 10 -6 moles per liter of rhodamine ethanol solution. The sample to be tested is adsorbed on the surface of the metal particles in the Raman scattering substrate 120. Please refer to FIG. 6. FIG. 6 shows a sample of a carbon nanotube film formed by a carbon nanotube and a metal particle in the detection system 100 and a sample of a carbon nanotube film formed by a carbon nanotube in the detection system 100. Raman spectral characteristics obtained when ×10 -3 moles of pyridine aqueous solution per liter. As can be seen from the figure, the Raman scattering peak of the pyridine is stronger than that in the detection system 100, and the vibration mode of each chemical bond of the pyridine can be clearly distinguished. Please refer to FIG. 7. FIG. 7 is a sample of a carbon nanotube composite film formed by a carbon nanotube and a metal particle in the detection system 100 and a sample for testing a carbon nanotube film formed by the carbon nanotube in the detection system 100. A Raman spectral characteristic obtained when 10 to 6 moles per liter of rhodamine ethanol solution. As can be seen from the figure, although the molecule of rhodamine is a fluorescent molecule, usually the Raman signal of the fluorescent molecule is masked by the fluorescent background, but the Raman scattering peak in the detection system 100 is stronger than that which can be significantly enhanced. .

該拉曼散射基底120包括一奈米碳管複合膜122,該奈米碳管複合膜122包括複數具有較小尺寸之奈米碳管,且該奈米碳管具有較大之比表面積,因此,該金屬顆粒能夠於該奈米碳管複合膜表面密集排佈,從而使單位面積上之金屬顆粒數目較多,即使單位面積上之金屬顆粒之密度較大。從而使該拉曼散射基底120具有較好之穩定性與靈敏性。 The Raman scattering substrate 120 includes a carbon nanotube composite film 122 comprising a plurality of carbon nanotubes having a smaller size, and the carbon nanotubes have a larger specific surface area, thus The metal particles can be densely arranged on the surface of the carbon nanotube composite film, so that the number of metal particles per unit area is large, even if the density of the metal particles per unit area is large. Thereby, the Raman scattering substrate 120 has better stability and sensitivity.

該拉曼散射基底100中之奈米碳管複合膜122包括複數具有較小尺寸及較大之比表面積之奈米碳管,且相鄰奈米碳管之間之間隙比較均勻且比較小。從而能夠使設置於奈米碳管膜表面之複數金屬顆粒均勻、密集排佈且不容易團聚。因此,用該拉曼散射基底100製作之拉曼檢測系統,具有廣泛之應用範圍和很高之靈敏度,可用來表徵各種分子之結構資訊。具體地,其可檢測濃度大於1×10-9摩爾每升之溶液樣品。 The carbon nanotube composite membrane 122 in the Raman scattering substrate 100 includes a plurality of carbon nanotubes having a smaller size and a larger specific surface area, and the gap between adjacent carbon nanotubes is relatively uniform and relatively small. Thereby, the plurality of metal particles disposed on the surface of the carbon nanotube film can be uniformly and densely arranged and not easily agglomerated. Therefore, the Raman detection system fabricated using the Raman scattering substrate 100 has a wide range of applications and high sensitivity, and can be used to characterize structural information of various molecules. Specifically, it can detect a solution sample having a concentration greater than 1 x 10 -9 moles per liter.

請參閱圖8,本發明第二實施例提供一種檢測系統200,其包括一發射模塊210、一拉曼散射基底220及一接收模塊230。該發射模塊210發射一光束到該拉曼散射基底220;該光束經由該拉曼散射基底220進行散射,形成散射光;該接收模塊230用於收集從該拉曼散射基底220散射之散射光,形成一拉曼光譜特徵圖。 Referring to FIG. 8 , a second embodiment of the present invention provides a detection system 200 including a transmitting module 210 , a Raman scattering substrate 220 , and a receiving module 230 . The transmitting module 210 emits a light beam to the Raman scattering substrate 220; the light beam is scattered through the Raman scattering substrate 220 to form scattered light; and the receiving module 230 is configured to collect scattered light scattered from the Raman scattering substrate 220, A Raman spectral feature map is formed.

該拉曼散射基底220,其包括一框架221及一奈米碳管複合膜222。該框架221固定於該奈米碳管複合膜222四週用於固定該奈米碳管複合膜222。該奈米碳管複合膜222包括由複數奈米碳管形成之至少一奈米碳管膜、形成於該奈米碳管表面之金屬顆粒及設置於該金屬顆粒與奈米碳管表面之間之緩衝層。該複數奈米碳管均勻排佈、相互平行且通過凡德瓦爾力相結合,該複數奈米碳管組成至少一自支撐之奈米碳管膜。 The Raman scattering substrate 220 includes a frame 221 and a carbon nanotube composite film 222. The frame 221 is fixed around the carbon nanotube composite membrane 222 for fixing the carbon nanotube composite membrane 222. The carbon nanotube composite membrane 222 includes at least one carbon nanotube film formed by a plurality of carbon nanotubes, metal particles formed on the surface of the carbon nanotube, and disposed between the metal particles and the surface of the carbon nanotube The buffer layer. The plurality of carbon nanotubes are evenly arranged, parallel to each other and combined by a van der Waals force, and the plurality of carbon nanotubes constitute at least one self-supporting carbon nanotube film.

本發明實施例提供之檢測系統200,其結構與原理與第一實施例提供之檢測系統100基本相同,其主要區別在於,該發射模塊210照射該拉曼散射基底220之光強係本發明第一實施例中發射模塊110照射該拉曼散射基底120之光強之四分之一。該拉曼散射基底220進一步包括一緩衝層設置於該金屬顆粒與奈米碳管表面之間,優選地,該緩衝層包覆每一奈米碳管表面,該每一奈米碳管表面均具有一緩衝層。該奈米碳管表面包覆緩衝層後形成之結構仍為一管狀,僅管徑增大。該緩衝層之材料為氧化物,該氧化物包括二氧化矽或氧化鎂。該緩衝層之厚度於10奈米~100奈米之間,優選地,該緩衝層 之厚度於15奈米~30奈米之間。在本實施例中,該緩衝層之材料為二氧化矽,其厚度為20奈米。該緩衝層用於隔絕該金屬顆粒與該奈米碳管,阻止金屬顆粒與奈米碳管之間之電子轉移。同時,通過設置該緩衝層,使該金屬顆粒具有較均勻之沈積面,該金屬顆粒於各個方向受力較勻稱,因此能夠使該金屬顆粒之曲率半徑之均勻性更好,從而使金屬顆粒更接近球形。可以理解,當該拉曼散射基底220不包括緩衝層時,該金屬顆粒直接設置於奈米碳管上,其沿奈米碳管生長方向之長軸半徑較大。 The detection system 200 provided by the embodiment of the present invention has the same structure and principle as the detection system 100 provided by the first embodiment. The main difference is that the emission module 210 illuminates the light intensity of the Raman scattering substrate 220. In one embodiment, the emission module 110 illuminates a quarter of the intensity of the Raman scattering substrate 120. The Raman scattering substrate 220 further includes a buffer layer disposed between the metal particles and the surface of the carbon nanotubes. Preferably, the buffer layer covers the surface of each of the carbon nanotubes, and the surface of each of the carbon nanotubes is Has a buffer layer. The structure formed after the surface of the carbon nanotube is coated with the buffer layer is still a tubular shape, and only the diameter of the tube is increased. The material of the buffer layer is an oxide comprising cerium oxide or magnesium oxide. The buffer layer has a thickness of between 10 nm and 100 nm, preferably the buffer layer The thickness is between 15 nm and 30 nm. In this embodiment, the buffer layer is made of cerium oxide and has a thickness of 20 nm. The buffer layer is used to insulate the metal particles from the carbon nanotubes and prevent electron transfer between the metal particles and the carbon nanotubes. At the same time, by providing the buffer layer, the metal particles have a relatively uniform deposition surface, and the metal particles are relatively well-balanced in all directions, so that the uniformity of the radius of curvature of the metal particles can be made better, thereby making the metal particles more uniform. Close to the sphere. It can be understood that when the Raman scattering substrate 220 does not include a buffer layer, the metal particles are directly disposed on the carbon nanotubes, and the radius of the long axis along the growth direction of the carbon nanotubes is large.

請參照圖9,為本實施例奈米碳管複合膜222之透射電鏡照片,該奈米碳管複合膜222中之複數奈米碳管形成有兩個層疊且交叉設置之奈米碳管膜。該複數奈米碳管外表面間隔設置有多晶結構之銀顆粒,該銀顆粒之粒徑於18奈米~22奈米之間;於該奈米碳管外表面與銀顆粒之間還形成有厚度為20奈米之二氧化矽緩衝層;同一奈米碳管表面,相鄰兩個銀顆粒之間之間隙於1奈米~5奈米之間。對比本發明第一實施例中之圖5,本發明實施例中之銀顆粒由於具有較均勻之之沈積面,即其曲率半徑更均勻,即該銀顆粒之形狀更接近球狀。 Referring to FIG. 9, a transmission electron micrograph of the carbon nanotube composite film 222 of the present embodiment is formed. The plurality of carbon nanotubes in the carbon nanotube composite film 222 are formed with two stacked and cross-shaped carbon nanotube films. . The outer surface of the plurality of carbon nanotubes is spaced apart by a silver particle having a polycrystalline structure, and the particle size of the silver particle is between 18 nm and 22 nm; and an outer surface of the carbon nanotube is formed between the outer surface of the carbon nanotube and the silver particle. There is a buffer layer of 20 nm thick ceria; on the surface of the same carbon nanotube, the gap between two adjacent silver particles is between 1 nm and 5 nm. Comparing Fig. 5 in the first embodiment of the present invention, the silver particles in the embodiment of the present invention have a more uniform deposition surface, that is, the radius of curvature thereof is more uniform, that is, the shape of the silver particles is closer to a spherical shape.

請參閱圖10,為本實施例中檢測系統200中由奈米碳管、緩衝層、金屬顆粒形成之奈米碳管複合膜222與由奈米碳管形成之奈米碳管膜檢測待測樣品為2.5×10-3摩爾每升之吡啶水溶液時所得到之拉曼光譜特性圖。請參閱圖11,為本實施例中檢測系統200中之拉曼散射基底中由奈米碳管、緩衝層、 金屬顆粒形成之奈米碳管複合膜與由奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時之拉曼光譜特性圖。 Referring to FIG. 10, in the detection system 200, the carbon nanotube composite film 222 formed by the carbon nanotubes, the buffer layer and the metal particles in the detection system 200 and the carbon nanotube film formed by the carbon nanotubes are tested. A Raman spectral characteristic diagram obtained when 2.5 x 10 -3 moles of pyridine aqueous solution per liter. Please refer to FIG. 11 , which is a carbon nanotube composite film formed by a carbon nanotube, a buffer layer and a metal particle in a Raman scattering substrate in the detection system 200 of the present embodiment, and a carbon nanotube film formed from a carbon nanotube. A Raman spectral characteristic diagram of the sample to be tested is 10 -6 moles per liter of rhodamine ethanol solution.

相對於本發明第一實施例檢測系統100,本發明實施例檢測系統200中之奈米碳管複合膜222由於進一步包括一層緩衝層,該緩衝層設置於該金屬顆粒與奈米碳管表面之間。通過設置該緩衝層,使該金屬顆粒設置於該緩衝層上而非直接設置於該奈米碳管表面,能夠使該金屬顆粒具有較均勻之沈積面,以使該金屬顆粒於各個方向受力較勻稱,曲率半徑之均勻性更好,使該金屬顆粒更容易產生表面等離子共振激發,因此該檢測系統200得到之拉曼光譜特性圖更為清晰,增強效應更明顯。具體地,該緩衝層由絕緣材料製成,優選地,該緩衝層之材料為氧化物,如二氧化矽、氧化鎂等;該緩衝層之厚度於10奈米~100奈米之間,優選地,該緩衝層之厚度於15奈米~30奈米之間。在本實施例中,該緩衝層之材料為二氧化矽,其厚度為20奈米。請參閱圖12,為10-6摩爾每升若丹明乙醇溶液分別於第一實施例檢測系統100及第二實施例檢測系統200檢測時得到之拉曼光譜特性圖之對比圖。通過對比圖可看出,由於設置該緩衝層後,該金屬顆粒更容易產生表面等離子共振激發,因此該檢測系統200得到之拉曼光譜特性圖更為清晰,增強效應更明顯。即使於該光束之光強只有第一實施例檢測系統100中光束之光強之四分之一。 The carbon nanotube composite film 222 in the detection system 200 of the embodiment of the present invention further includes a buffer layer disposed on the surface of the metal particle and the carbon nanotube tube. between. By disposing the buffer layer, the metal particles are disposed on the buffer layer instead of being directly disposed on the surface of the carbon nanotube, so that the metal particles have a relatively uniform deposition surface, so that the metal particles are stressed in various directions. The uniformity of the radius of curvature is better, and the metal particles are more likely to generate surface plasmon resonance excitation. Therefore, the Raman spectral characteristic map obtained by the detection system 200 is clearer and the enhancement effect is more obvious. Specifically, the buffer layer is made of an insulating material. Preferably, the buffer layer is made of an oxide such as cerium oxide, magnesium oxide or the like; and the buffer layer has a thickness of between 10 nm and 100 nm, preferably The thickness of the buffer layer is between 15 nm and 30 nm. In this embodiment, the buffer layer is made of cerium oxide and has a thickness of 20 nm. Referring to FIG. 12, a comparison chart of Raman spectral characteristics obtained when the 10-6 moles per liter of rhodamine ethanol solution is detected in the first embodiment detection system 100 and the second embodiment detection system 200, respectively. It can be seen from the comparison chart that since the metal particles are more likely to generate surface plasmon resonance excitation after the buffer layer is disposed, the Raman spectral characteristic map obtained by the detection system 200 is clearer and the enhancement effect is more obvious. Even if the intensity of the beam is only one quarter of the intensity of the beam in the detection system 100 of the first embodiment.

請參閱圖13及圖14,圖13為本發明第三實施例提供一種檢測 系統300,其包括一發射模塊310、一拉曼散射基底320及一接收模塊330。該發射模塊310用於發射一光束到該拉曼散射基底320;該光束經由該拉曼散射基底320進行散射,形成散射光;該接收模塊330用於收集從該拉曼散射基底320散射之散射光,形成一拉曼光譜特徵圖。 Please refer to FIG. 13 and FIG. 14. FIG. 13 is a diagram of a third embodiment of the present invention. The system 300 includes a transmitting module 310, a Raman scattering substrate 320, and a receiving module 330. The transmitting module 310 is configured to emit a light beam to the Raman scattering substrate 320; the light beam is scattered through the Raman scattering substrate 320 to form scattered light; and the receiving module 330 is configured to collect scattering scattered from the Raman scattering substrate 320. Light forms a Raman spectral feature map.

該拉曼散射基底320包括一基底321及一奈米碳管複合膜322形成於該基底321表面。該基底321用於支撐該奈米碳管複合膜322,該基底321之結構與材料不限,優選地,該基底321具有較好之光透過率。該光束中部分光子直接照射到該基低321上,如果該基底321具有較好之光透過率,則這部分光子將直接射出;反之,這部分將被該基底321反射,發射過來之光子部分還可能照射到該奈米碳管複合膜322中之奈米碳管而形成散射光,該散射光將會對具待測樣品分子結構資訊之散射光干擾。從而不利於該拉曼檢測系統300對待測樣品之檢測。該奈米碳管複合膜322包括由複數奈米碳管形成之奈米碳管膜及設置於該奈米碳管膜表面之複數金屬顆粒。該複數奈米碳管均勻排佈、大致相互平行且通過凡德瓦爾力相結合。 The Raman scattering substrate 320 includes a substrate 321 and a carbon nanotube composite film 322 formed on the surface of the substrate 321 . The substrate 321 is used to support the carbon nanotube composite film 322. The structure and material of the substrate 321 are not limited. Preferably, the substrate 321 has a good light transmittance. A portion of the photons in the beam are directly incident on the base low 321 . If the substrate 321 has a good light transmittance, the photons will be directly emitted; otherwise, the portion will be reflected by the substrate 321 and the photons emitted therefrom. It is also possible to illuminate the carbon nanotubes in the carbon nanotube composite membrane 322 to form scattered light that will interfere with the scattered light of the molecular structure of the sample to be tested. This is detrimental to the detection of the sample to be tested by the Raman detection system 300. The carbon nanotube composite membrane 322 includes a carbon nanotube membrane formed of a plurality of carbon nanotubes and a plurality of metal particles disposed on the surface of the carbon nanotube membrane. The plurality of carbon nanotubes are evenly arranged, substantially parallel to each other and joined by van der Waals forces.

本發明實施例提供之檢測系統300,其結構與原理與第一實施例提供之檢測系統100基本相同,其主要區別在於,該奈米碳管膜中之複數奈米碳管大致垂直在於該奈米碳管膜之表面,即該複數奈米碳管以陣列之方式排佈且基本垂直於該奈米碳管膜表面,從而形成一奈米碳管陣列。該金屬顆粒基本 設置於該奈米碳管陣列遠離該基底321之端部從而形成一散射表面,即該金屬顆粒大致設置於該奈米碳管陣列與該基底321相對之一端。請參閱圖14,在本實施例中,該金屬顆粒之粒徑於10奈米~50奈米之間,且每一奈米碳管端部均設置有一金屬顆粒。 The detection system 300 provided by the embodiment of the present invention has the same structure and principle as the detection system 100 provided by the first embodiment, and the main difference is that the plurality of carbon nanotubes in the carbon nanotube film are substantially perpendicular to the nanometer. The surface of the carbon nanotube film, i.e., the plurality of carbon nanotubes, is arranged in an array and substantially perpendicular to the surface of the carbon nanotube film to form an array of carbon nanotubes. The metal particles are basically The carbon nanotube array is disposed away from the end of the substrate 321 to form a scattering surface, that is, the metal particles are disposed substantially at one end of the carbon nanotube array opposite to the substrate 321 . Referring to FIG. 14, in the embodiment, the metal particles have a particle diameter of between 10 nm and 50 nm, and each of the carbon nanotubes is provided with a metal particle at the end.

該奈米碳管可為單壁奈米碳管、雙璧奈米碳管或多壁奈米碳管。請參閱圖15,為本實施例中檢測系統300中由多壁奈米碳管、金屬顆粒形成之奈米碳管複合膜320與由多壁奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得對之拉曼光譜特性圖。該金屬顆粒為粒徑於13奈米~17奈米之間之銀顆粒。請參閱圖16,為本實施例中檢測系統300中由單壁奈米碳管、13奈米~17奈米金屬顆粒形成之奈米碳管複合膜322、圖13中拉曼散射基底中由單壁奈米碳管、28奈米~32奈米金屬顆粒形成之奈米碳管複合膜322及由單壁奈米碳管形成之奈米碳管膜檢測待測樣品為10-6摩爾每升之若丹明乙醇溶液時所得到之拉曼光譜特性圖。 The carbon nanotubes can be single-walled carbon nanotubes, double-twisted carbon nanotubes or multi-walled carbon nanotubes. Referring to FIG. 15, in the detection system 300, the carbon nanotube composite film 320 formed by the multi-walled carbon nanotubes and the metal particles and the carbon nanotube film formed by the multi-walled carbon nanotubes are detected in the detection system 300. The Raman spectral characteristics obtained when the sample was measured in 10-6 moles per liter of rhodamine ethanol solution. The metal particles are silver particles having a particle diameter of between 13 nm and 17 nm. Referring to FIG. 16, in the detection system 300, a carbon nanotube composite film 322 formed of a single-walled carbon nanotube, a 13 nm to 17 nm metal particle, and a Raman scattering substrate in FIG. Single-walled carbon nanotubes, nanocarbon tube composite membrane 322 formed by 28 nm to 32 nm metal particles, and nanocarbon tube membrane formed by single-walled carbon nanotubes, the sample to be tested is 10-6 moles per sample. Raman spectral characteristics obtained when the rhodamine ethanol solution is ascended.

從圖15及圖16可看出,在該金屬顆粒之粒徑相當之情況下,由單壁奈米碳管組成之奈米碳管複合膜322較由多壁奈米碳管組成之奈米碳管複合膜322所得到拉曼光譜特性圖,其對待測樣品之拉曼光譜之增強效應更為明顯。這係因為由多壁奈米碳管組成之奈米碳管膜之密度略大於由單壁奈米碳管組成之奈米碳管膜,從而導致單位面積內之碳元素增多,從而使得奈米碳管複合膜322之光透射率下降,增加了未與待測 樣品分子碰撞之光子之散射數量。當該光束中之光子未與待測樣品分子碰撞,而直接經由該奈米碳管散射時,該部分散射光將具有奈米碳管中之分子結構資訊,從而對具有該待測樣品分子結構資訊之散射光造成干擾。即導致由奈米碳管形成之奈米碳管膜所得到之待測樣品之拉曼光譜強度較大,從而使該奈米碳管複合膜322所得到之拉曼光譜強度與該奈米碳管膜所得到之拉曼光譜強度之對比度下降,從而降低了對待測樣品之拉曼光譜之增強效應。 As can be seen from Fig. 15 and Fig. 16, in the case where the particle diameter of the metal particles is equivalent, the carbon nanotube composite film 322 composed of a single-walled carbon nanotube is composed of a nanometer composed of a multi-walled carbon nanotube. The Raman spectral characteristic of the carbon nanotube composite film 322 is more obvious, and the enhancement effect of the Raman spectrum of the sample to be tested is more obvious. This is because the density of the carbon nanotube film composed of multi-walled carbon nanotubes is slightly larger than that of the carbon nanotube film composed of single-walled carbon nanotubes, resulting in an increase in carbon content per unit area, thereby making nano The light transmittance of the carbon tube composite film 322 is decreased, and the increase is not detected. The amount of photon scattering by the collision of sample molecules. When the photon in the beam does not collide with the sample molecule to be tested and is directly scattered through the carbon nanotube, the partially scattered light will have molecular structure information in the carbon nanotube, thereby having the molecular structure of the sample to be tested. The scattered light of the information causes interference. That is, the Raman spectrum intensity of the sample to be tested obtained by the carbon nanotube film formed by the carbon nanotubes is large, so that the Raman spectral intensity obtained by the carbon nanotube composite film 322 and the carbon nanotubes are obtained. The contrast of the Raman spectral intensity obtained by the film is reduced, thereby reducing the enhancement effect of the Raman spectrum of the sample to be tested.

該拉曼散射基底包括一奈米碳管複合膜,該奈米碳管複合膜包括複數具有較小尺寸和較大比表面積之奈米碳管。因此,該金屬能夠以較小之粒徑密集排佈於該奈米碳管複合膜表面。從而使該拉曼散射基底具有較好之穩定性與靈敏性。 The Raman scattering substrate comprises a carbon nanotube composite membrane comprising a plurality of carbon nanotubes having a smaller size and a larger specific surface area. Therefore, the metal can be densely arranged on the surface of the carbon nanotube composite film with a small particle diameter. Thereby, the Raman scattering substrate has better stability and sensitivity.

綜上所述,本發明確已符合發明專利之要件,遂依法提出專利申請。惟,以上所述者僅為本發明之較佳實施例,自不能以此限制本案之申請專利範圍。舉凡習知本案技藝之人士援依本發明之精神所作之等效修飾或變化,皆應涵蓋於以下申請專利範圍內。 In summary, the present invention has indeed met the requirements of the invention patent, and has filed a patent application according to law. However, the above description is only a preferred embodiment of the present invention, and it is not possible to limit the scope of the patent application of the present invention. Equivalent modifications or variations made by those skilled in the art in light of the spirit of the invention are intended to be included within the scope of the following claims.

100‧‧‧檢測系統 100‧‧‧Detection system

110‧‧‧發射模塊 110‧‧‧Transmission module

120‧‧‧拉曼散射基底 120‧‧‧ Raman scattering substrate

121‧‧‧支撐結構 121‧‧‧Support structure

122‧‧‧奈米碳管複合膜 122‧‧‧Nano Carbon Tube Composite Film

130‧‧‧接收模塊 130‧‧‧ receiving module

Claims (23)

一種拉曼散射基底,其改進在於,其包括一奈米碳管複合膜,該奈米碳管複合膜包括至少一奈米碳管膜及複數金屬顆粒,該奈米碳管膜包括複數奈米碳管,該複數金屬顆粒設置於該複數奈米碳管表面,該奈米碳管膜中之複數奈米碳管沿一個方向擇優取向排列。 A Raman scattering substrate is improved in that it comprises a carbon nanotube composite membrane comprising at least one carbon nanotube membrane and a plurality of metal particles, the carbon nanotube membrane comprising a plurality of nanometer membranes The carbon tube, the plurality of metal particles are disposed on the surface of the plurality of carbon nanotubes, and the plurality of carbon nanotubes in the carbon nanotube film are arranged in a preferred orientation in one direction. 如請求項第1項所述之拉曼散射基底,其中,該複數奈米碳管均勻分佈,相鄰之奈米碳管通過凡德瓦爾力結合。 The Raman scattering substrate according to Item 1, wherein the plurality of carbon nanotubes are uniformly distributed, and the adjacent carbon nanotubes are combined by a van der Waals force. 如請求項第1項所述之拉曼散射基底,其中,該奈米碳管膜為一自支撐結構。 The Raman scattering substrate of claim 1, wherein the carbon nanotube film is a self-supporting structure. 如請求項第1項所述之拉曼散射基底,其中,該拉曼散射基底進一步包括一框架,該奈米碳管複合膜通過該框架至少部分懸空設置。 The Raman scattering substrate of claim 1, wherein the Raman scattering substrate further comprises a frame through which the carbon nanotube composite film is at least partially suspended. 如請求項第4項所述之拉曼散射基底,其中,該奈米碳管複合膜包括多層奈米碳管膜層疊設置。 The Raman scattering substrate of claim 4, wherein the carbon nanotube composite film comprises a multilayered carbon nanotube film laminate arrangement. 如請求項第1項所述之拉曼散射基底,其中,該奈米碳管膜中之複數奈米碳管大致相互平行且大致平行於該奈米碳管膜表面,該複數奈米碳管通過凡德瓦爾力首尾相連。 The Raman scattering substrate of claim 1, wherein the plurality of carbon nanotubes in the carbon nanotube film are substantially parallel to each other and substantially parallel to the surface of the carbon nanotube film, the plurality of carbon nanotubes Connected end to end by Van der Valli. 如請求項第1項所述之拉曼散射基底,其中,該拉曼散射基底進一步包括一基底,該基底具有一表面,該奈米碳管複合膜覆蓋該表面。 The Raman scattering substrate of claim 1, wherein the Raman scattering substrate further comprises a substrate having a surface, the carbon nanotube composite film covering the surface. 如請求項第7項所述之拉曼散射基底,其中,該奈米碳管膜 中之複數奈米碳管大致垂直於該奈米碳管膜之表面,且由凡德瓦爾力結合。 The Raman scattering substrate of claim 7, wherein the carbon nanotube film The plurality of carbon nanotubes are substantially perpendicular to the surface of the carbon nanotube film and are combined by Van der Waals force. 如請求項第1項所述之拉曼散射基底,其中,每一奈米碳管表面均設置有至少一金屬顆粒。 The Raman scattering substrate of claim 1, wherein each of the carbon nanotube surfaces is provided with at least one metal particle. 如請求項第1項所述之拉曼散射基底,其中,該複數金屬顆粒間隔設置。 The Raman scattering substrate of claim 1, wherein the plurality of metal particles are spaced apart. 如請求項第1項所述之拉曼散射基底,其中,相鄰兩個金屬顆粒之間之間隙於1奈米~15奈米之間。 The Raman scattering substrate according to Item 1, wherein the gap between two adjacent metal particles is between 1 nm and 15 nm. 如請求項第11項所述之拉曼散射基底,其中,相鄰兩個金屬顆粒之間之間隙於1奈米~5奈米之間。 The Raman scattering substrate according to claim 11, wherein a gap between two adjacent metal particles is between 1 nm and 5 nm. 如請求項第1項所述之拉曼散射基底,其中,該金屬顆粒之粒徑於10奈米~50奈米之間。 The Raman scattering substrate according to Item 1, wherein the metal particles have a particle diameter of between 10 nm and 50 nm. 如請求項第1項所述之拉曼散射基底,其中,該金屬顆粒之粒徑於18奈米~22奈米之間。 The Raman scattering substrate according to Item 1, wherein the metal particles have a particle diameter of between 18 nm and 22 nm. 如請求項第1項所述之拉曼散射基底,其中,該金屬顆粒之材料為過渡金屬或貴金屬。 The Raman scattering substrate according to Item 1, wherein the material of the metal particles is a transition metal or a noble metal. 如請求項第1項所述之拉曼散射基底,其中,該金屬顆粒為多晶結構之銀顆粒,其粒徑於18奈米~22奈米之間,相鄰兩個銀顆粒之間之間隙於1奈米~5奈米之間。 The Raman scattering substrate according to Item 1, wherein the metal particles are polycrystalline silver particles having a particle diameter of between 18 nm and 22 nm, between two adjacent silver particles. The gap is between 1 nm and 5 nm. 如請求項第1項所述之拉曼散射基底,其中,該奈米碳管複合膜進一步包括一緩衝層設置於該金屬顆粒與奈米碳管之間。 The Raman scattering substrate of claim 1, wherein the carbon nanotube composite film further comprises a buffer layer disposed between the metal particles and the carbon nanotubes. 如請求項第17項所述之拉曼散射基底,其中,該緩衝層之材料為氧化物。 The Raman scattering substrate of claim 17, wherein the material of the buffer layer is an oxide. 如請求項第17項所述之拉曼散射基底,其中,該緩衝層之厚度於10奈米~100奈米之間。 The Raman scattering substrate of claim 17, wherein the buffer layer has a thickness between 10 nm and 100 nm. 如請求項第17項所述之拉曼散射基底,其中,該緩衝層之材料為二氧化矽,厚度為18奈米~22奈米。 The Raman scattering substrate according to Item 17, wherein the buffer layer is made of cerium oxide and has a thickness of from 18 nm to 22 nm. 一種拉曼散射基底,其改進在於,其包括一奈米碳管複合膜,該奈米碳管複合膜包括至少一奈米碳管膜、複數緩衝層及複數金屬顆粒,該奈米碳管膜包括複數奈米碳管,該複數緩衝層設置於該複數奈米碳管表面,該複數金屬顆粒設置於該複數緩衝層表面,該奈米碳管膜中之複數奈米碳管沿一個方向擇優取向排列。 A Raman scattering substrate, which is improved in that it comprises a carbon nanotube composite membrane comprising at least one carbon nanotube membrane, a plurality of buffer layers and a plurality of metal particles, the carbon nanotube membrane The plurality of carbon nanotubes are disposed on the surface of the plurality of carbon nanotubes, and the plurality of metal particles are disposed on the surface of the plurality of buffer layers, and the plurality of carbon nanotubes in the carbon nanotube film are preferentially oriented in one direction Orientation. 一種拉曼散射基底,其改進在於,其包括一奈米碳管複合膜,該奈米碳管複合膜包括由兩層奈米碳管膜層疊交叉設置形成之一膜狀結構,一緩衝層設置於該膜狀結構表面,複數金屬顆粒間隔設置於該緩衝層背向該膜狀結構之表面,該奈米碳管膜包括複數奈米碳管通過凡德瓦爾力首尾相連且基本沿同一方向擇優取向排列,該奈米碳管膜中之複數奈米碳管沿一個方向擇優取向排列。 A Raman scattering substrate, which is improved in that it comprises a carbon nanotube composite film comprising a film structure formed by laminating two layers of carbon nanotube film layers, a buffer layer setting On the surface of the film structure, a plurality of metal particles are spaced apart from the surface of the buffer layer facing away from the film structure, and the carbon nanotube film comprises a plurality of carbon nanotubes connected end to end by van der Waals force and is substantially optimized in the same direction Oriented, the plurality of carbon nanotubes in the carbon nanotube film are arranged in a preferred orientation in one direction. 一種拉曼檢測系統,其包括一發射模塊、一拉曼散射基底及一接收模塊;該發射模塊用於向該拉曼散射基底發射一光束;該拉曼散射基底用於將該發射模塊發射過來之光束進行散射;該接收模塊用於收集從該拉曼散射基底散射之散射光,形成一拉曼光譜特徵圖; 其改進在於,該拉曼散射基底包括一奈米碳管複合膜,該奈米碳管複合膜包括至少一奈米碳管膜及複數金屬顆粒,該奈米碳管膜包括複數均勻分佈之奈米碳管,相鄰之奈米碳管通過凡德瓦爾力結合,該複數金屬顆粒設置於該複數奈米碳管表面,該奈米碳管膜中之複數奈米碳管沿一個方向擇優取向排列。 A Raman detection system includes a transmitting module, a Raman scattering substrate and a receiving module; the transmitting module is configured to emit a light beam to the Raman scattering substrate; the Raman scattering substrate is used to transmit the transmitting module The light beam is scattered; the receiving module is configured to collect scattered light scattered from the Raman scattering substrate to form a Raman spectral characteristic map; The improvement is that the Raman scattering substrate comprises a carbon nanotube composite membrane comprising at least one carbon nanotube membrane and a plurality of metal particles, the nanocarbon membrane comprising a plurality of uniformly distributed a carbon carbon tube, the adjacent carbon nanotubes are combined by a van der Waals force, and the plurality of metal particles are disposed on the surface of the plurality of carbon nanotubes, and the plurality of carbon nanotubes in the carbon nanotube film are preferentially oriented in one direction arrangement.
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