WO2015146036A1 - Dispositif de spectroscopie raman amélioré - Google Patents

Dispositif de spectroscopie raman amélioré Download PDF

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Publication number
WO2015146036A1
WO2015146036A1 PCT/JP2015/001357 JP2015001357W WO2015146036A1 WO 2015146036 A1 WO2015146036 A1 WO 2015146036A1 JP 2015001357 W JP2015001357 W JP 2015001357W WO 2015146036 A1 WO2015146036 A1 WO 2015146036A1
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Prior art keywords
flow path
flow
convex structure
excitation light
metal fine
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PCT/JP2015/001357
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English (en)
Japanese (ja)
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昇吾 山添
芽実 塩田
納谷　昌之
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富士フイルム株式会社
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Publication of WO2015146036A1 publication Critical patent/WO2015146036A1/fr

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/01—Arrangements or apparatus for facilitating the optical investigation
    • G01N21/03—Cuvette constructions
    • G01N21/05—Flow-through cuvettes
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65—Raman scattering
    • G01N21/658—Raman scattering enhancement Raman, e.g. surface plasmons

Definitions

  • the present invention relates to an enhanced Raman spectroscopic apparatus including a photoelectric field enhancement device having a fine metal concavo-convex structure capable of inducing localized plasmons, and in particular, includes a photoelectric field enhancement device in a flow path.
  • the present invention relates to an enhanced Raman spectrometer.
  • Raman spectroscopy is a method of obtaining a spectrum of Raman scattered light (Raman spectrum) by dispersing scattered light obtained by irradiating a substance with single wavelength light, and is used for identification of a substance.
  • Raman spectroscopy there is Raman spectroscopy using a photoelectric field enhanced by localized plasmon resonance, called surface enhanced Raman (SERS), in order to enhance weak Raman scattered light.
  • SERS substrate An electric field enhancement device (so-called SERS substrate) used for such enhanced Raman spectroscopy, which produces an electric field enhancement effect by a localized plasmon resonance phenomenon on a metal surface is known.
  • Raman spectroscopy when a substance is in contact with a metal body, particularly a metal body with nano-order irregularities on its surface, a surface-enhanced electric field due to localized plasmon resonance is generated, and the surface of the metal body is contacted.
  • This utilizes the principle that the Raman scattered light intensity of the sample is enhanced.
  • Raman light which is orders of magnitude smaller than fluorescence
  • a high-power excitation light source and a measurement system that required a long detection time can be used for a short time of several seconds or less with a low-power semiconductor laser by using a surface-enhanced electric field. Since the measurement system can be used, the effect is very large.
  • Non-Patent Document 1 a metal fine concavo-convex structure is formed in a hollow fiber and filled with a liquid containing a specimen, thereby increasing the area where the metal fine concavo-convex structure and the specimen are in contact with each other and performing highly sensitive SERS detection. ing.
  • Patent Document 1 or Non-Patent Document 2 a metal fine concavo-convex structure is formed in a flow path device, and SERS measurement is performed by flowing a liquid.
  • the following two means can be considered.
  • One is to increase the area where the specimen is in contact with the metal fine concavo-convex structure in order to increase the probability of capturing the specimen signal approaching the metal surface with a low probability.
  • the second is a method of causing the specimen to flow and forcibly approaching the surface of the metal fine concavo-convex structure.
  • Non-Patent Document 1 since the fine concavo-convex structure is formed on the entire inner wall in the hollow fiber, the area where the specimen comes into contact with the fine concavo-convex structure can be increased.
  • a capillary phenomenon is used as a method for introducing a liquid into the hollow fiber. The measurement is performed after injecting the liquid, the specimen does not move greatly, and is not actively approaching the metal surface. In addition, gas molecules cannot be detected because capillary action does not occur in gas.
  • Patent Document 1 detection is performed while flowing the specimen, and an effect of bringing the specimen closer to the surface of the fine concavo-convex structure is obtained.
  • the area where the excitation and SERS signals are detected is a limited area (spot) collected by the objective lens, and it cannot be said that sufficient S / N is obtained.
  • the present invention has been made in view of the above circumstances, and an object thereof is to provide an enhanced Raman spectroscopic device capable of detecting a signal with high S / N regardless of gas or liquid.
  • the enhanced Raman spectroscopic device of the present invention includes a flow channel for flowing down a fluid sample, a flow channel device having a metal fine concavo-convex structure provided on at least a part of the inner wall of the flow channel, A flow mechanism for flowing a fluid sample in the flow path of the flow path device; An excitation optical system for irradiating excitation light toward the metal fine concavo-convex structure in the flow path; A detection unit that detects light generated by irradiation of excitation light, The excitation optical system is characterized in that the excitation light is extended and irradiated in the direction in which the flow path of the flow path device extends.
  • the metal fine concavo-convex structure has a fine concavo-convex structure that can generate localized plasmons when irradiated with excitation light.
  • the fine concavo-convex structure capable of generating localized plasmons is generally a concavo-convex structure in which the average size and average pitch of the convex portions and concave portions forming the concavo-convex structure are smaller than the wavelength of the excitation light.
  • the direction in which the flow path of the flow path device extends is the flow direction of the fluid sample, and the metal fine concavo-convex structure is provided in a predetermined region along the direction in which the flow path extends.
  • the excitation optical system may condense the excitation light on the metal fine concavo-convex structure in a rectangular or elliptical shape from a direction perpendicular to the direction in which the flow path extends.
  • the excitation optical system moves the excitation light from the bent portion toward the flow channel portion where the metal fine uneven structure is formed in the direction in which the flow channel portion extends.
  • the excitation light may be irradiated with the optical axes aligned.
  • a protrusion structure for disturbing the flow of the fluid sample is disposed in the flow path portion where the metal fine concavo-convex structure is formed.
  • two or more different sensing regions may be provided.
  • Two or more different sensing regions may be regions that cause different Raman shifts for the same specimen, or have affinity for different specimens and enable multiple specimen detection. May be.
  • the fine metal concavo-convex structure may have two or more regions made of different metals as two or more different sensing regions.
  • the metal fine concavo-convex structure may have two or more regions having different surface presence / absence and / or types on the concavo-convex structure as two or more different sensing regions.
  • the surface modification may be an inorganic layer or an organic layer, and may be appropriately selected according to the analyte during sample flow.
  • the enhanced Raman spectroscopic device of the present invention includes a flow channel for flowing a fluid sample, a flow channel device having a metal fine uneven structure provided on at least a part of the inner wall of the flow channel, and a fluid in the flow channel of the flow channel device. Since the flow mechanism for flowing the sample is provided and the fluid sample containing the specimen can be measured while flowing, an effect of forcibly bringing the specimen closer to the surface of the metal fine concavo-convex structure can be obtained. In addition, since the fluid mechanism is provided, the fluid sample can be flowed down regardless of whether the fluid sample is liquid or gas.
  • the excitation optical system extends and irradiates the excitation light in the direction in which the flow path of the flow path device extends, the detectable area can be increased as compared with the spot irradiation of the excitation light. Therefore, highly sensitive sensing is possible even for a sample having a low affinity with a metal.
  • FIG. 1 is a diagram illustrating a schematic configuration of an enhanced Raman spectroscopic device according to a first embodiment.
  • FIG. It is a figure which shows schematic structure of the flow-path system of the enhancement Raman spectroscopy apparatus shown in FIG.
  • FIG. 3 is a cross-sectional view taken along the line IIIA-IIIA, a cross-sectional view taken along the line IIIB-IIIB of the flow channel device shown in FIG. It is a perspective view which shows a SERS board
  • substrate shown in FIG. 6 is a schematic cross-sectional view showing a flow path device of design change example 1.
  • FIG. 1 It is a schematic diagram which shows the structure which increases a pumping light direction using a cylindrical flow-path device. It is a figure which shows schematic structure of the enhanced Raman spectroscopy apparatus which concerns on 3rd Embodiment. It is a figure which shows typically the relationship between the optical axis Laxis of excitation light, and the flow axis Faxis of a flow path, and the light quantity distribution of the excitation light in a flow axis direction. It is a cross-sectional schematic diagram which shows the flow-path device of the example of a design change.
  • FIG. 1 is a diagram showing a schematic configuration of an enhanced Raman spectroscopic apparatus 1 according to a first embodiment of the present invention.
  • the enhanced Raman spectroscopic apparatus 1 detects the Raman light generated from the subject by irradiating the flow path device 11 with the flow path system 11 including a flow path device 11 partially having a metal fine concavo-convex structure and the flow path device 11.
  • An optical sensing system 20 is provided.
  • the optical sensing system 20 includes an excitation optical system 20a and a Raman light detection optical system 20b.
  • the excitation optical system 20a is an optical system for irradiating excitation light toward a metal fine concavo-convex structure in a flow channel device to be described later, and the Raman light detection optical system 20b detects Raman light generated by irradiation of excitation light. This is an optical system including a spectroscopic detector 29.
  • the optical sensing system 20 includes a laser light source 21 that emits laser light, a collimating lens 22 that collimates the laser light from the light source 21, a laser line filter 23 for narrowing the spectrum of the laser light, A cylindrical lens 24 for ellipticalizing the laser light, a dichroic mirror 25 that reflects excitation light that is laser light and transmits Raman light having a longer wavelength than the excitation light, and excitation light that is reflected by the dichroic mirror 25 is described later.
  • the excitation optical system 20a includes a laser light source 21, a collimator lens 22, a laser line filter 23, a cylindrical lens 24, a dichroic mirror 25, and a condenser lens 26.
  • the Raman light detection optical system 20b includes a condenser lens 26 and a dichroic mirror. 25, a sharp cut long wave length pass filter 27, a lens 28 and a spectral detector 29.
  • the dichroic mirror 25 and the condenser lens 26 serve as both elements of the excitation optical system 20a and the Raman light detection optical system 20b.
  • FIG. 2 is a diagram showing a schematic configuration of the flow path system 10.
  • the flow path system 10 includes a flow path device 11 having a metal fine concavo-convex structure therein, a suction pump 13 which is a flow mechanism for flowing a fluid sample, and a waste liquid container for storing a sucked liquid sample. 14, a storage container 15 for storing a liquid sample is provided, and the storage container 15, the flow channel device 11, the waste liquid container 14, and the suction pump 13 are connected by a tube 16 in this order.
  • the liquid sample in the storage container 15 flows through the flow path 11 a in the flow path device 11 via the tube 16 and further flows to the waste liquid container 14 via the tube 16.
  • FIG. 3 shows a IIIA-IIIA sectional view (A) and a IIIB-IIIB sectional view (B) of the flow channel device 11 shown in FIG.
  • the flow channel device 11 of the present embodiment includes a flow channel 11a that allows a fluid sample to flow down, and a metal fine concavo-convex structure 11b provided on at least a part of the inner wall of the flow channel 11a.
  • the flow channel device 11 includes a flow channel member 17 having a groove 17 a formed along the length direction, and a SERS substrate 18 serving as a cover plate that covers the groove 17 a of the flow channel member 17.
  • the SERS substrate 18 includes a transparent base material 18a, a transparent fine uneven structure layer 18b and a metal fine uneven structure layer 18c formed on one surface of the transparent base material 18a.
  • the inner wall of the flow path 11a is constituted by the wall surface of the groove 17a and the base material 18a of the SERS substrate 18.
  • the flow path member 17 is formed by forming a 1 mm ⁇ 2 mm square groove in the center of a rod made of PDMS (polydimethylsiloxane) of 10 mm ⁇ 10 mm ⁇ 50 mm, for example, and the groove becomes a flow path.
  • the SERS substrate 18 is, for example, a SERS substrate described in Japanese Patent Application Laid-Open No. 2012-063293, and uses a boehmite formed on a glass substrate having a size of 10 mm ⁇ 50 mm ⁇ thickness 1 mm, and gold is deposited thereon. Can do.
  • FIG. 4 is a perspective view showing the SERS substrate 18, and FIG. 5 is an enlarged view of a part V of the side surface of the SERS substrate 18 shown in FIG.
  • the SERS substrate 18 includes a transparent base material 18a, a transparent fine uneven structure layer 18b, and a metal film 18c formed on the surface of the fine uneven structure.
  • the metal film 18 c is formed along the surface of the transparent fine concavo-convex structure layer to constitute a metal fine concavo-convex structure, and light irradiated to the metal fine concavo-convex structure (hereinafter referred to as excitation light and ) Induces localized plasmon resonance, and this localized plasmon resonance generates an enhanced photoelectric field on the surface of the metal fine concavo-convex structure.
  • the metal fine concavo-convex structure is a fine concavo-convex structure in which the average size and average pitch of the concavo-convex convex portions are shorter than the wavelength of the excitation light. Anything can be used.
  • the metal fine concavo-convex structure has an average depth of 200 nm or less from the top of the convex portion to the bottom of the adjacent concave portion, and an average pitch between the vertices of the nearest adjacent convex portions that are separated from the concave portion.
  • the metal film 18c may be made of a metal that can generate localized plasmons when irradiated with excitation light.
  • the metal film 18c is made of Au, Ag, Cu, Al, Pt, or an alloy containing these as a main component. It consists of at least one metal selected from the group. In particular, Au or Ag is preferable.
  • the film thickness of the metal film 18c is such that when it is formed on the surface of the transparent fine concavo-convex structure layer 18b, the metal fine concavo-convex structure can maintain a concavo-convex shape capable of generating localized plasmons upon irradiation with excitation light.
  • the thickness is not particularly limited, but is preferably 10 to 100 nm.
  • the transparent fine concavo-convex structure layer 18b is preferably made of a material mainly composed of alumina hydrate, and specifically, boehmite or buyer light is preferable.
  • a method for manufacturing the SERS substrate 18 will be described with reference to FIG.
  • a plate-like transparent substrate (transparent substrate) 18a is prepared, and the transparent substrate 18a is washed with pure water. Thereafter, an aluminum 8 film having a thickness of about several tens of nanometers is formed on the surface of the transparent substrate 18a by sputtering. Thereafter, the pure base material 18a with aluminum 8 is submerged in boiling pure water and taken out after a few minutes (about 5 minutes). By this boiling treatment (boehmite treatment), the aluminum 8 becomes transparent and becomes a transparent fine concavo-convex structure layer 18b made of a boehmite layer. By depositing the metal film 18c on the transparent fine uneven structure layer 18b, the SERS substrate 18 having the metal fine uneven structure on the surface can be obtained.
  • the formation method of the metal fine concavo-convex structure is a very simple method. According to the above method, even if the transparent substrate is not plate-shaped, for example, the metal fine concavo-convex structure is applied to a curved surface by the same method. The structure can be easily formed.
  • the laser light emitted from the light source 21 is stretched in one direction by the cylindrical lens 24 through the lens 22 and the filter 23 and is shaped into an ellipse, and then is formed by the dichroic mirror 25.
  • the light is reflected toward the flow channel device 11 and irradiated to the metal fine concavo-convex structure 11 b of the flow channel device 11 by the lens 26.
  • the extending direction of the laser light (long axis direction of the elliptical irradiation field) and the extending direction of the flow path 11a coincide with each other, and the excitation light extends over a wide range of the flow path. Irradiated at the same time.
  • the Raman light from the specimen existing in the excitation light irradiation range is enhanced by the SERS substrate and detected by the spectroscopic detector 29 of the Raman light detection optical system 20b.
  • 3C is a graph showing the amount of excitation light in the flow direction of the flow path device 11. As shown in FIG. 3C, the excitation light is irradiated with the excitation light stretched over a wide range in the flow direction.
  • the fluid sample is caused to flow in the flow channel 11a of the flow channel device 11, thereby increasing the chance that the specimen in the flow sample is brought close to the metal microstructure, and wide.
  • the range with excitation light By irradiating the range with excitation light, more Raman light can be detected, and highly sensitive detection is possible.
  • FIG. 7 shows a cross-sectional view (A) in the length direction and a cross-sectional view (B) perpendicular to the length direction of the flow path device 31 according to the first design change example.
  • the flow path device 31 shown in FIG. 7 is provided with a protrusion 19a in the flow path, and is configured to generate a turbulent flow in the fluid flowing through the flow path.
  • the protrusion 19a is provided on the groove bottom surface of the flow path member 19 having a groove serving as a flow path.
  • FIG. 8 is a cross-sectional view in the length direction of the flow path device 32 according to the second design change example.
  • the flow channel device 32 shown in FIG. 8 is partially different from the above-described flow channel device 11 in the configuration of the SERS substrate.
  • the SERS substrate 18A serving as a lid plate of the flow path device 32 has two regions made of metals having different metal fine concavo-convex structures.
  • One region 33a of the surface of the transparent fine concavo-convex structure layer 18b provided on the surface of the transparent base material 18a has a structure including metal films 18c and 18d made of gold and the other region 33b made of platinum, respectively.
  • FIG. 9 is a cross-sectional view in the length direction of the flow path device 34 of the design modification example 3.
  • the flow channel device 34 shown in FIG. 9 is partly different from the above flow channel device 11 in the configuration of the SERS substrate.
  • the SERS substrate 18B serving as the lid plate of the flow channel device 34 has two regions 35a and 35b having different affinity for the specimen on the metal fine concavo-convex structure.
  • the metal film 18c is uniformly formed on the surface of the transparent fine concavo-convex structure layer 18b provided on the surface of the transparent substrate 18a, and the modification 18e by SAM (self-assembled monolayer) is applied only to one region 35b. Has been.
  • the surface modification is not limited to SAM, and may be an inorganic layer. Further, in this example, the region 35a not subjected to surface modification and the region 35b subjected to surface modification are provided, but two or more different types of surface modification regions may be provided. Signals from the different regions 35a and 35b are simultaneously detected by the spectroscopic detector, and are divided into spectral shapes for analysis.
  • FIG. 10 shows a cross-sectional view (A) in the length direction and a cross-sectional view (B) perpendicular to the length direction of the flow path device 36 of the design modification example 4.
  • the flow channel device 36 shown in FIG. 10 is a cylindrical flow channel device.
  • the cylindrical channel device 36 is configured by bonding semi-cylindrical channel members 36A and 36B.
  • the cylindrical flow channel device has a cylindrical flow channel 36a inside, and is provided with a fine metal uneven structure 36b over almost the entire inner wall of the flow channel 36a.
  • the metal fine concavo-convex structure 36b can be produced by the fine concavo-convex structure formation and the metal film deposition process in the above-described SERS substrate production.
  • the cylindrical flow path 36a is provided with projections 37 at predetermined intervals in the flow path length direction so as to cause turbulence in the fluid flowing in the flow path 36a.
  • this cylindrical flow path device 36 it becomes possible to excite the enhanced field efficiently by applying a coating for reflecting excitation light to the inner wall surface or the outer wall surface.
  • a coating for reflecting excitation light for example, as shown in FIG. 11, an excitation light reflecting coating 39 is applied to the outer peripheral region of the cylindrical flow channel device 36 except for the excitation light incident region.
  • the flow channel device 36 is passed through the lens 12. Since the irradiated excitation light is reflected inside the flow path, the excitation effect can be enhanced.
  • FIG. 12 shows a schematic configuration diagram of the enhanced Raman spectroscopic device 2 according to the second embodiment of the present invention.
  • the same elements as those of the device 1 of the first embodiment are denoted by the same reference numerals, detailed description thereof will be omitted, and differences from the device 1 of the first embodiment will be mainly described.
  • the flow path device 40 is configured to be excited from two directions. Since the excitation light density is decreased by irradiating the excitation light with ovalization, the decrease in the excitation light density is compensated by increasing the number of light sources.
  • the spectral detector 29 is shared, and the Raman light that has passed through the lens 28 of each detection optical system 20b is collected by the line bundle fiber 30, and the two bundle fibers 30 are in the middle. And then connected to the spectral detector 29.
  • FIG. 13 shows a cross-sectional view (A) in the flow path length direction of the flow path device 40 used in this embodiment (A) and a cross-sectional view (B) perpendicular to the length direction.
  • the flow channel device 40 includes a flow channel member 41 having an opening 41 a serving as a flow channel and two SERS substrates 18 disposed above and below the flow channel member 41. That is, the flow channel device 40 has a configuration in which sensing regions each having a fine metal relief structure are formed above and below the flow channel.
  • FIG. 14 shows a cross-sectional view (A) in the length direction and a cross-sectional view (B) perpendicular to the length direction of the flow path device 42 of the design change example.
  • the flow path device 42 shown in FIG. 14 is provided with protrusions 43a in the flow path, and is configured to generate turbulence in the fluid flowing through the flow path.
  • the protrusion 43 a is provided in the shape of a bridge that connects the wall surfaces in the opening serving as the flow path of the flow path member 43.
  • the channel device 42 is provided with a projection 43a for generating turbulent flow between the SERS substrates inside the channel, so that the specimen in the fluid sample approaches the metal surface of the SERS substrate constituting the upper and lower surfaces of the channel. It has a higher probability and has a preferable structure due to higher sensitivity.
  • the cylindrical flow path device 36 shown in FIG. 10 is used and the excitation light is irradiated from four directions as shown in FIG. 15, the excitation direction (excitation light quantity) is further increased and the sensitivity is increased. can do.
  • FIG. 16 shows a schematic configuration diagram of an enhanced Raman spectroscopic device 3 according to a third embodiment of the present invention.
  • the optical sensing system 120 does not include a cylindrical lens, does not extend the excitation light itself, and irradiates the channel device with circular excitation light. It is a configuration.
  • the shape of the flow path device 135 is different from that of the flow path device 11 of the first embodiment. It has a cylindrical channel and a bent portion 136 where the flow direction of the fluid changes. More specifically, the flow channel device 135 has a configuration in which a flow channel portion 139 extending in a direction orthogonal to a flow channel portion 138 having a fine uneven structure formed on the inner wall is connected by a bent portion 136. 135a is bent at a right angle at a bent portion 136. A wall surface 137 (one side surface of the bent portion 136) perpendicular to the direction in which the flow path portion 138 extends has a flat surface that constitutes a condensing window for excitation light. Such a special structure can be manufactured by die-molding PDMS.
  • the flow path device can be assembled after being formed as two or more parts.
  • a metal fine concavo-convex structure 135 b is formed on the inner wall of the flow path device 135.
  • the metal fine concavo-convex structure 135b is manufactured in the same manner as the SERS substrate.
  • the transparent fine concavo-convex structure film is formed by forming a film containing aluminum on the inner wall surface and then performing hot water treatment. In this method, gold is deposited on the fine concavo-convex structure film. At this time, before the film containing aluminum is formed, the inner wall is coated with silver. This silver coating does not change particularly even after the subsequent formation of a film containing aluminum, hot water treatment or the like.
  • FIG. 17 is a diagram schematically showing the relationship between the optical axis Laxis of the excitation light and the flow axis Faxis of the flow path, and the light quantity distribution of the excitation light in the flow axis direction.
  • the flow axis Faxis of the fluid in the flow path device 135 is indicated by a broken line
  • the optical axis Laxis of the excitation light is indicated by a one-dot chain line.
  • the flow axis Faxis changes at a right angle at the bent portion 136.
  • Excitation light is irradiated into the flow path through the condensing lens 26 of the optical sensing system 120. At this time, the excitation light passes from the side wall 137 of the bent portion 136 into the flow path 135a so that the optical axis Laxis of the excitation light coincides with the fluid flow axis Faxis in the flow path portion 138 where the metal fine uneven structure 135b is formed. Is incident on.
  • the excitation light is guided in the excitation light channel by the silver coating in the channel, and as a result, the excitation light is stretched and irradiated in the extending direction of the channel.
  • excitation light is irradiated to the metal fine concavo-convex structure 135b over a wide range of the flow path portion 138.
  • the extension irradiation does not irradiate the excitation light irradiation field shape as an ellipse or rectangle in a uniaxial direction, but spreads the irradiation region in the direction in which the flow path extends by guiding the light. (Stretching) configuration. That is, in the present invention, the extension irradiation of excitation light includes the case where the excitation light is guided in the flow path in this way to irradiate a wide range of metal fine concavo-convex structures with excitation light. At this time, as shown in FIG. 17, the amount of excitation light is greatest on the light incident side in the flow path, and the amount of excitation light decreases as the distance from the incident position increases.
  • FIG. 18 shows a flow path device 140 of a design change example.
  • the channel device 140 has a cylindrical channel and a bent portion 145 in which the fluid flow direction changes.
  • the flow path 140a has a widened portion 142 that spreads in the vicinity of the bent portion 145, and one surface 143 of the corner of the bent portion is released, and the lid is covered by the condenser lens 26 of the optical sensing system 120. Yes. It is possible to avoid the influence of reflection, aberration and the like due to the side wall of the flow path.
  • a protrusion that generates a turbulent flow Is preferably provided.
  • a fine concavo-convex structure made of different metals is formed on the SERS substrate, or that the metal surface is modified with an organic or inorganic material.

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Abstract

Le problème décrit par la présente invention est de pourvoir à un dispositif de spectroscopie Raman amélioré pouvant détecter des signaux avec un rapport S/B élevé, indépendamment d'un gaz ou d'un liquide. La solution selon l'invention porte sur un dispositif de spectroscopie Raman amélioré qui comprend : un dispositif (11) de trajet d'écoulement ayant un trajet d'écoulement (11a) dans lequel un échantillon de fluide est amené à s'écouler, et une structure irrégulière fine métallique (11b) prévue sur au moins une partie d'une paroi interne du trajet d'écoulement (11a); un mécanisme d'écoulement (13) permettant d'amener l'échantillon de fluide à s'écouler à l'intérieur du trajet d'écoulement (11a) du dispositif (11) de trajet d'écoulement; un système optique d'excitation (20a) permettant d'émettre une lumière d'excitation vers la structure irrégulière fine métallique (11b) dans le trajet d'écoulement (11a); et une unité de détection (29) qui détecte la lumière générée par l'émission de la lumière d'excitation. Le système optique d'excitation (20a) est conçu de manière à émettre la lumière d'excitation de façon à s'étendre dans une direction le long de laquelle s'étend le trajet d'écoulement (11a) du dispositif (11) de trajet d'écoulement.
PCT/JP2015/001357 2014-03-24 2015-03-12 Dispositif de spectroscopie raman amélioré WO2015146036A1 (fr)

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JP2014-060114 2014-03-24
JP2014060114A JP2015184114A (ja) 2014-03-24 2014-03-24 増強ラマン分光装置

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2020203761A1 (fr) * 2019-03-29 2020-10-08 キヤノン株式会社 Film d'absorption de lumière / d'isolation thermique, élément d'absorption de lumière / d'isolation thermique, article et leurs procédés de fabrication
WO2021256320A1 (fr) * 2020-06-16 2021-12-23 国立研究開発法人理化学研究所 Appareil de spectrométrie par diffusion raman et procédé de spectrométrie par diffusion raman
US11555788B2 (en) * 2020-03-15 2023-01-17 Alexander K. Pourshalchi Nondestructive fluid sensing

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