Optical Waveguide, and SPR Sensor Cell and Colorimetric Sensor Cell Which Use Optical Waveguide

TECHNICAL FIELD

The present invention relates to an optical waveguide, and an SPR sensor cell and a colorimetric sensor cell each using the optical waveguide.

BACKGROUND ART

Hitherto, in the fields of chemical analysis, biochemical analysis, and the like, a surface plasmon resonance (SPR) sensor including an optical fiber has been used. In the SPR sensor including an optical fiber, a metal thin film is formed on an outer circumferential surface of a tip end portion of the optical fiber, and an analysis sample is fixed to the optical fiber into which light is guided. Among the light to be guided, light having a particular wavelength generates surface plasmon resonance in the metal thin film, and light intensity thereof is attenuated. In such SPR sensor, the wavelength of the light generating surface plasmon resonance generally varies depending on, for example, a refractive index of an analysis sample to be fixed to the optical fiber. Therefore, when a wavelength at which light intensity is attenuated after the generation of surface plasmon resonance is measured, the wavelength of the light generating surface plasmon resonance can be identified. Further, when a change in the wavelength at which light intensity is attenuated is detected, it can be confirmed that the wavelength of the light generating surface plasmon resonance has changed, and hence a change in refractive index of the analysis sample can be confirmed. As a result, such SPR sensor can be used for various chemical analyses and biochemical analyses, such as measurement of a sample concentration and detection of an immunoreaction.

In the SPR sensor including an optical fiber, the tip end portion of the optical fiber has a fine cylindrical shape, and hence there is a problem in that it is difficult to form the metal thin film and fix an analysis sample to the optical fiber. In order to solve the problem, for example, there has been proposed an SPR sensor cell including a core through which light is transmitted and a clad covering the core, in which a through-hole extending to a surface of the core is formed at a predetermined position of the clad, and a metal thin film is formed on the surface of the core at a position corresponding to the through-hole (for example, Patent Literature 1). In such SPR sensor cell, it is easy to form the metal thin film for generating surface plasmon resonance on the surface of the core and fix the analysis sample onto the surface. However, in such SPR sensor, a crack may be formed in a surface of the cladding during a process of forming the cladding by curing a varnish. The crack is more liable to occur when the cladding is formed through use of a halogen-containing resin material (for example, Patent Literature 2).

CITATION LIST
Patent Literature

[PTL 1] JP 2000-19100 A

[PTL 2] JP 2010-84150 A

SUMMARY OF INVENTION
Technical Problem

The present invention has been made in order to solve the problem of the related art described above, and an object of the present invention is to provide an optical waveguide in which the occurrence of a crack in a cladding layer is prevented, and an SPR sensor cell and a colorimetric sensor cell each using the optical waveguide.

Solution to Problem

As a result of investigations on the mechanism of crack occurrence, which have been made by the inventors of the present invention, it was presumed that a crack may occur because, owing to a high surface hardness of a resin for forming a cladding, the stress of curing shrinkage of the resin, or the like is liable to be concentrated on the surface of the cladding. Then, the inventors have found that the occurrence of a crack can be prevented by adjusting the surface hardness of the cladding to a predetermined range. Thus, the inventors have completed the present invention.

That is, according to one embodiment of the present invention, there is provided an optical waveguide including: a cladding layer; and a core layer buried in the cladding layer so that at least one surface of the core layer is exposed, in which the cladding layer has a surface hardness of HB to 2H.

In one embodiment of the present invention, the cladding layer includes a resin for forming a cladding layer and particles dispersed in the resin for forming a cladding layer.

In one embodiment of the present invention, a filling ratio of the particles in the cladding layer is 2% to 50%.

In one embodiment of the present invention, an average particle diameter (φ) of the particles is 200 nm to 2.5 μm.

In one embodiment of the present invention, the cladding layer has a storage modulus of 0.3 GPa or less.

In one embodiment of the present invention, the resin for forming a cladding layer contains a halogen.

According to another aspect of the present invention, there is provided an SPR sensor cell. The SPR sensor cell of the present invention includes the optical waveguide.

According to another aspect of the present invention, there is provided a colorimetric sensor cell. The colorimetric sensor cell of the present invention includes the optical waveguide.

Advantageous Effects Of Invention

According to the present invention, the optical waveguide in which the occurrence of a crack in a cladding layer is prevented, and the SPR sensor cell and the colorimetric sensor cell each using the optical waveguide can be provided.

BRIEF DESCRIPTION OF DRAWINGS

FIG. 1 is a schematic perspective view for illustrating an optical waveguide according to a preferred embodiment of the present invention.

FIG. 2 is a schematic perspective view of an SPR sensor cell according to the preferred embodiment of the present invention.

FIG. 3 is a schematic sectional view of the SPR sensor cell illustrated in FIG. 2 taken along a line Ia-Ia.

FIG. 4 is a schematic perspective view of a colorimetric sensor cell according to the preferred embodiment of the present invention.

FIG. 5 is a schematic sectional view of the colorimetric sensor cell illustrated in FIG. 4 taken along a line Ib-Ib.

FIGS. 6 are schematic views for illustrating an example of a method of manufacturing the optical waveguide of the present invention.

DESCRIPTION OF EMBODIMENTS

[A. Optical Waveguide]

An optical waveguide of the present invention includes a cladding layer having a predetermined surface hardness, and a core layer buried in the cladding layer so that at least one surface of the core layer is exposed. An optical loss (propagation loss) of the optical waveguide of the present invention at a wavelength of 660 nm is, for example, less than 2.6 dB/cm, preferably 2.0 dB/cm or less, more preferably 1.5 dB/cm or less. When the optical loss falls within this range, the optical waveguide can be suitably used as a detection unit of a sensor cell, such as an SPR sensor cell or a colorimetric sensor cell to be described later. The optical loss is measured using a cutback technique.

FIG. 1 is a schematic perspective view for illustrating an optical waveguide according to a preferred embodiment of the present invention. In the illustrated example, an optical waveguide 100 includes a cladding layer 11 and a core layer 12 buried in the cladding layer 11 so that an incidence port, an output port, and an upper surface of the core layer 12 are exposed. The optical waveguide 100 is formed into a flat plate-like shape having a substantially rectangular shape in a plan view. The thickness of the cladding layer (thickness from the upper surface of the core layer) is, for example, 5 μm to 400 μm. Unlike the illustrated example, the upper surface and a lower surface of the core layer may be exposed from the cladding layer.

The cladding layer 11 preferably includes a resin for forming a cladding layer and particles dispersed in the resin for forming a cladding layer. When the particles are dispersed in the cladding layer, in the case of forming the cladding layer through use of a high-hardness resin (e.g., a resin having a surface hardness of 4H or more after curing), such as a halogen-containing resin, the surface hardness can be adjusted to a predetermined range to be described later without a significant increase in storage modulus. It is considered that the cladding layer consequently has an appropriate softness, and hence a stress due to curing shrinkage is dispersed and the occurrence of a crack is prevented.

Any suitable particles may be used as the particles. For example, the particles are formed of a material having a refractive index of preferably 1.40 to 3.00, more preferably 1.43 to 2.60. Using such a material has an advantage in that a refractive index of the cladding layer is easily adjusted to fall within a desired range. Further, for example, the particles are formed of a material having an extinction coefficient of preferably 0.1 or less, more preferably 0. When the particles are formed of a material having such extinction coefficient, the influence of an increase in temperature of the particles due to light absorption can be avoided. The refractive index as used herein means a refractive index at a wavelength of 830 nm. Further, the extinction coefficient as used herein means an extinction coefficient at a wavelength of 830 nm.

A metal and an inorganic oxide are given as specific examples of a material for forming the particles. Preferred examples of the metal may include titanium, tantalum, aluminum, zinc, chromium, and iron. In addition, preferred examples of the inorganic oxide may include metal oxides (such as titanium oxide (TiO₂), tantalum oxide (Ta₂O₅), aluminum oxide (Al₂O₃), zinc oxide (ZnO), chromium oxide (Cr₂O₃), iron oxide (Fe₂O₃), and copper oxide (CuO)) and metalloid oxides (such as boron oxide (B₂O₃), silicon oxide (SiO₂), and germanium oxide (GeO₂)). The particles may be used alone or in combination.

An average particle diameter (φ) of the particles is, for example, 10 nm to 5 μm. The lower limit of the average particle diameter is preferably 200 nm, more preferably 300 nm. Further, the upper limit of the average particle diameter is preferably 2.5 μm, more preferably 2.0 μm. With such an average particle diameter, the surface hardness of the cladding layer can be easily controlled to fall within a predetermined range to be described later. The average particle diameter as used herein means a median diameter. The average particle diameter of the particles in the cladding layer can be obtained based on, for example, laser diffraction/scattering particle size distribution measurement, or a volume-based particle size distribution that is obtained from a particle size distribution determined through image processing of an SEM image of a cross section of the cladding layer.

Any suitable resin capable of forming the cladding layer having a lower refractive index than that of the core layer described later may be used as the resin for forming a cladding layer, and a halogen-containing resin is preferably used. Specific examples of the halogen-containing resin include: fluorine atom-containing resins such as polytetrafluoroethylene, a tetrafluoroethylene-hexafluoropropylene copolymer, a fluorinated epoxy resin, a fluorinated polyimide resin, a fluorinated polyamide resin, a fluorinated acrylic resin, a fluorinated polyurethane resin, and a fluorinated siloxane resin; chlorine atom-containing resins such as a vinyl chloride resin, a vinyl chloride-ethylene copolymer, and a chlorinated polyolefin resin; and modified products thereof. From the viewpoint of, for example, obtaining a desired refractive index, a fluorine atom-containing resin is preferred. They may be used alone or in combination. Any such resin may be preferably blended with a photosensitizing agent so as to be used as a photosensitive material.

The halogen-containing resin has a halogen content of preferably 35 wt % or more, more preferably 40 wt % or more, still more preferably 50 wt % or more. When the halogen content falls within such range, a cladding layer having a low refractive index can be easily obtained. Meanwhile, the upper limit of the halogen content is preferably 78 wt %. When the upper limit is more than 78 wt %, the cladding layer may undergo liquefaction or gasification, thereby failing to maintain the shape of the cladding layer.

A refractive index of the resin for forming a cladding layer is lower than the refractive index of the particles. A difference between the refractive index of the resin for forming a cladding layer and the refractive index of the particles is preferably 0.03 or more, more preferably 0.05 or more, still more preferably 0.07 or more, yet still more preferably 0.10 or more.

The refractive index of the resin for forming a cladding layer is preferably 1.42 or less, more preferably less than 1.40, still more preferably 1.38 or less.

A filling ratio of the particles in the cladding layer 11 is, for example, 1% to 50%. The lower limit of the filling ratio is preferably 2%, more preferably 3%, still more preferably 5%. Further, the upper limit of the filling ratio is preferably 30%, more preferably 25%. In each of the case where the filling ratio is excessively small and the case where the filling ratio is excessively large, the effect of the addition of the particles to lower the surface hardness of the cladding layer may not be obtained sufficiently. On the other hand, when the filling ratio is, for example, 2% to 50%, the surface hardness of the cladding layer can be easily controlled to a predetermined range to be described later without a significant increase in storage modulus.

The cladding layer 11 has a surface hardness of HB to 2H, preferably F to 2H, more preferably H to 2H. When the surface hardness is more than 2H, a stress occurs inside the resin for forming a cladding layer due to its curing not relaxing, and the stress is concentrated on the surface, with the result that a crack is liable to occur. Meanwhile, when the surface hardness is less than HB, a problem may arise in, for example, that a flaw is liable to occur.

The cladding layer 11 has a storage modulus (25° C.) of preferably 0.3 GPa or less, more preferably 0.15 GPa to 0.3 GPa, still more preferably 0.16 GPa to 0.25 GPa. With such storage modulus, a stress due to curing shrinkage is suitably dispersed, and hence such storage modulus can contribute to the prevention of a crack.

The core layer 12 is formed substantially in a square column shape extending in a direction orthogonal to both a width direction and a thickness direction of the cladding layer 11, and is buried in an upper end portion substantially at the center of the width direction of the cladding layer 11. The direction in which the core layer 12 extends serves as a direction in which light is propagated in the optical waveguide.

The core layer 12 is arranged so that the upper surface thereof is flush with an upper surface of the cladding layer 11. A metal layer or a protective layer can be arranged efficiently only on an upper side of the core layer in the SPR sensor cell or the colorimetric sensor cell to be described later by arranging the core layer so that the upper surface thereof is flush with the upper surface of the cladding layer. Further, the core layer is arranged so that both end surfaces thereof in the extending direction are flush with both end surfaces of the cladding layer in the extending direction.

A refractive index (N_CO) of the core layer 12 can be set to any suitable value depending on intended use and the like. For example, when the optical waveguide 100 is applied to an SPR sensor cell, the refractive index (N_CO) of the core layer 12 is preferably 1.43 or less, more preferably less than 1.40, still more preferably 1.38 or less. When the refractive index of the core layer is set to 1.43 or less, the detection sensitivity can be markedly improved. The lower limit of the refractive index of the core layer is preferably 1.34. When the refractive index of the core layer is 1.34 or more, SPR can be excited even in an aqueous solution-based sample (refractive index of water: 1.33), and a generally used material can be used.

The refractive index (N_CO) of the core layer 12 is higher than the refractive index (N_CL) of the cladding layer 11. The difference (N_CO-N_CL) between the refractive index of the core layer and the refractive index of the cladding layer is preferably 0.010 or more, more preferably 0.020 or more, still more preferably 0.025 or more. When the difference between the refractive index of the core layer and the refractive index of the cladding layer falls within such range, the optical waveguide 100 can be set to the so-called multimode. Thus, the quantity of light transmitted through the optical waveguide can be increased, and the S/N ratio can be enhanced when the optical waveguide is applied to the SPR sensor cell or the colorimetric sensor cell to be described later. Further, the difference between the refractive index of the core layer and the refractive index of the cladding layer is preferably 0.15 or less, more preferably 0.10 or less, still more preferably 0.050 or less.

The thickness of the core layer 12 is, for example, 5 μm to 200 μm, preferably 20 μm to 200 μm. Further, the width of the core layer is, for example, 5 μm to 200 μm, preferably 20 μm to 200 μm. When the core layer has such thickness and/or width, the optical waveguide 100 can be set to the so-called multimode. Further, the length (waveguide length) of the core layer 12 is, for example, 2 mm to 50 mm, preferably 10 mm to 20 mm.

Any suitable material may be used as a material for forming the core layer 12 as long as the effects of the present invention can be obtained. For example, the core layer 12 may be formed of a resin that is similar to the resin for forming a cladding layer and is adjusted so as to have a higher refractive index than that of the cladding layer.

One core layer is illustrated in FIG. 1, but the number of the core layers may be changed depending on the purpose. Specifically, a plurality of core layers may be formed at predetermined intervals in a width direction of the cladding layer. Further, any suitable shape (for example, a semi-cylindrical shape or a convex columnar shape) may be employed as the shape of the core layer depending on purposes.

[B. SPR Sensor Cell]

FIG. 2 is a schematic perspective view for illustrating an SPR sensor cell according to the preferred embodiment of the present invention. FIG. 3 is a schematic sectional view of the SPR sensor cell illustrated in FIG. 2 taken along the line Ia-Ia.

An SPR sensor cell 200 has, as illustrated in FIG. 2 and FIG. 3, a bottomed frame shape having a substantially rectangular shape in a plan view, and includes: the optical waveguide 100 including the under-cladding layer 11 and the core layer 12 buried in the under-cladding layer 11 so that the upper surface of the core layer 12 is exposed; and a metal layer 20 for covering the under-cladding layer 11 and the core layer 12. The optical waveguide 100 and the metal layer 20 serve as a detection unit 210 configured to detect a state of a sample and/or a change thereof. In the illustrated embodiment, the SPR sensor cell 200 includes a sample placing portion 220 formed so as to be adjacent to the detection unit 210. The sample placing portion 220 is defined by an over-cladding layer 30. The over-cladding layer 30 may be omitted as long as the sample placing portion 220 can be formed appropriately. In the sample placing portion 220, a sample (for example, a solution or powder) to be analyzed is placed so as to come into contact with the detection unit (substantially, the metal layer).

The optical waveguide 100 is as described in the above-mentioned item A.

As illustrated in FIG. 2 and FIG. 3, the metal layer 20 is formed so as to uniformly cover at least a part of the upper surfaces of the under-cladding layer 11 and the core layer 12. As necessary, an easy-adhesion layer (not shown) may be formed between the under-cladding layer and the metal layer, and between the core layer and the metal layer. By forming the easy-adhesion layer, the under-cladding layer and the core layer can be fixed to the metal layer firmly.

As a material for forming the metal layer, there may be given gold, silver, platinum, copper, aluminum, and alloys thereof. The metal layer may be a single layer, or may have a laminate structure of two or more layers. The thickness (total thickness of all the layers in the case of the laminate structure) of the metal layer is preferably 20 nm to 70 nm, more preferably 30 nm to 60 nm.

As a material for forming the easy-adhesion layer, there may be typically given chromium or titanium. The thickness of the easy-adhesion layer is preferably 1 nm to 5 nm.

As illustrated in FIG. 2, the over-cladding layer 30 is formed into the shape of a frame having a rectangular shape in a plan view so that an outer periphery of the over-cladding layer 30 becomes substantially flush with an outer periphery of the optical waveguide 100 in a plan view, on the upper surface of the optical waveguide 100. A portion surrounded by the upper surfaces of the optical waveguide 100 and the over-cladding layer 30 is partitioned as the sample placing portion 220. By placing a sample in the partitioned portion, the metal layer of the detection unit 210 and the sample come into contact with each other so that detection can be performed. Further, by forming such partitioned portion, a sample can be easily placed on the surface of the metal layer, and hence the operability can be enhanced.

As a material for forming the over-cladding layer 30, for example, there may be given the materials for forming the core layer and the under-cladding layer, and silicone rubber. The thickness of the over-cladding layer is preferably 5 μm to 2,000 μm, more preferably 25 μm to 200 μm. The refractive index of the over-cladding layer is preferably lower than the refractive index of the core layer. In one embodiment, the refractive index of the over-cladding layer is equal to the refractive index of the under-cladding layer.

Although the SPR sensor cell according to the preferred embodiment of the present invention has been described above, the present invention is not limited thereto. For example, a protective layer may be arranged between the optical waveguide 100 and the metal layer 20. In this case, the protective layer may be formed as a thin film having the same shape as that of the optical waveguide in a plan view so as to completely cover the upper surface of the optical waveguide 100. When the protective layer is arranged, for example, in the case where the sample is liquid, the core layer and/or the cladding layer can be prevented from being swollen with the sample. As a material for forming the protective layer, for example, there are given silicon dioxide and aluminum oxide. Any such material may be preferably adjusted so as to have a lower refractive index than that of the core layer. The protective layer has a thickness of preferably 1 nm to 100 nm, more preferably 5 nm to 20 nm.

Further, a lid may be arranged on an upper portion of the SPR sensor cell 200 (sample placing portion 220). With such configuration, a sample can be prevented from coming into contact with ambient air. In addition, when the sample is a solution, a change in concentration caused by evaporation of a solvent can be prevented. When the lid is arranged, an injection port for injecting a liquid sample into the sample placing portion and a discharge port for discharging the liquid sample from the sample placing portion may be formed. With such configuration, the sample can be allowed to flow to be supplied to the sample placing portion continuously, and hence the characteristics of the sample can be measured continuously.

The above-mentioned embodiments may be combined appropriately.

An example of the manner of use of such SPR sensor cell 200 is described below.

First, a sample is placed in the sample placing portion 220 of the SPR sensor cell 200 so that the sample and the metal layer 20 are brought into contact with each other. Then, light from any suitable light source is guided to the SPR sensor cell 200 (core layer 12). The light guided to the SPR sensor cell 200 (core layer 12) is transmitted through the SPR sensor cell 200 (core layer 12) while repeating total reflection in the core layer 12, and part of the light enters the metal layer 20 on an upper surface of the core layer 12 and is attenuated by surface plasmon resonance. The light transmitted through and output from the SPR sensor cell 200 (core layer 12) is guided to any suitable optical measuring instrument. That is, the intensity of light having a wavelength generating surface plasmon resonance in the core layer 12 is attenuated in the light guided from the SPR sensor 200 to the optical measuring instrument. The wavelength of light generating surface plasmon resonance depends on, for example, the refractive index of the sample brought into contact with the metal layer 20. Therefore, through the detection of the attenuation of the light intensity of the light guided to the optical measuring instrument, the refractive index of the sample and a change thereof can be detected.

[C. Colorimetric Sensor Cell]

FIG. 4 is a schematic perspective view for illustrating a colorimetric sensor cell according to the preferred embodiment of the present invention. FIG. 5 is a schematic sectional view of the colorimetric sensor cell illustrated in FIG. 4 taken along the line Ib-Ib.

A colorimetric sensor cell 300 has, as illustrated in FIG. 4 and FIG. 5, a bottomed frame shape having a substantially rectangular shape in a plan view, and includes the optical waveguide 100 including the under-cladding layer 11 and the core layer 12 buried in the under-cladding layer 11 so that the upper surface of the core layer 12 is exposed. The optical waveguide 100 serves as a detection unit 310 configured to detect a state of a sample and/or a change thereof. In the illustrated embodiment, the colorimetric sensor cell 300 further includes a protective layer 40 for covering the upper surface of the optical waveguide 100 and a sample placing portion 320 formed so as to be adjacent to the detection unit 310 through the protective layer 40. The protective layer 40 may be omitted depending on the purpose. The sample placing portion 320 is defined by the over-cladding layer 30. The over-cladding layer 30 may be omitted as long as the sample placing portion 320 can be formed appropriately. In the sample placing portion 320, a sample (for example, a solution or powder) to be analyzed is placed so as to come into contact with the detection unit (the protective layer 40 in the illustrated example). Further, although not illustrated, similarly to the SPR sensor cell described in the above-mentioned item B, a lid may be arranged on the colorimetric sensor cell 300 (sample placing portion 320).

The optical waveguide 100 is as described in the above-mentioned item A. Further, the over-cladding layer 30 and the protective layer 40 are as described in the above-mentioned item B.

An example of the manner of use of such colorimetric sensor cell 300 is described below.

First, a sample is placed in the sample placing portion 320 of the colorimetric sensor cell 300 so that the sample and the protective layer 40 are brought into contact with each other. Then, light from any suitable light source is guided to the colorimetric sensor cell 300 (core layer 12). The light guided to the colorimetric sensor cell 300 (core layer 12) is transmitted through the colorimetric sensor cell 300 (core layer 12) while repeating total reflection in the core layer 12. In addition, part of the light leaks out of the core layer 12 as an evanescent wave, and enters the sample on the upper surface of the core layer 12 through the protective layer 40 to be attenuated. The light that has been transmitted through the colorimetric sensor cell 300 (core layer 12) to be emitted is guided to any suitable light measuring instrument. That is, the intensity of light having a wavelength that is absorbed by the sample on the core layer 12 is attenuated in the light guided from the colorimetric sensor cell 300 to the light measuring instrument. The wavelength that is absorbed by the sample differs depending on, for example, a color of the sample placed on the colorimetric sensor cell 300, and hence the color of the sample and a change thereof can be detected through detection of the attenuation of the light intensity of the light guided to the light measuring instrument.

[D. Manufacturing Method]

Any suitable method may be used as a method of manufacturing the optical waveguide of the present invention. As a specific example of the method of producing the optical waveguide of the present invention, a method illustrated in FIG. 6 or a method illustrated in FIG. 3 of JP 2012-215541 A is given.

In the method illustrated in FIG. 6, first, as illustrated in FIG. 6(a), a material 12′ for forming a core layer is applied on a surface of a die 50 having a recessed portion corresponding to the shape of the core layer. Then, as illustrated in FIG. 6(b), a transfer film 60 is bonded onto the surface of the die 50 while the transfer film 60 is pressed in a predetermined direction with pressing means 70. Thus, the excessive material 12′ for forming a core layer is removed while the material 12′ for forming a core layer is filled into the recessed portion. After that, as illustrated in FIG. 6(c), the material 12′ for forming a core layer filled into the recessed portion is irradiated with ultraviolet rays to be cured. Thus, the core layer 12 is formed. In addition, as illustrated in FIG. 6(d), the transfer film 60 is peeled from the die 50, and the core layer 12 is thus transferred onto the transfer film 60.

Then, as illustrated in FIG. 6(e), a material 11′ for forming a cladding layer, which includes a resin for forming a cladding layer and particles dispersed in the resin as appropriate, is applied on the core layer 12 so as to cover the core layer 12. Alternatively, unlike the illustrated example, the material 11′ for forming a cladding layer may be applied on another support (for example, a PET film subjected to corona treatment) in advance, and the support and the transfer film 60 may be bonded to each other so that the material 11′ for forming a cladding layer covers the core layer 12. After that, as illustrated in FIG. 6(f), the material 11′ for forming a cladding layer is irradiated with ultraviolet rays to be cured. Thus, the cladding layer 11 is formed. Then, as illustrated in FIG. 6(g), the transfer film 60 is peeled to be removed and the resultant is flipped upside down. Thus, the optical waveguide including the core layer 12 buried in the cladding layer 11 is obtained.

The irradiation conditions for the ultraviolet rays can be appropriately set depending on the kinds of the materials. The materials may be heated as needed. The heating may be performed before the ultraviolet ray irradiation, after the ultraviolet ray irradiation, or simultaneously with the ultraviolet ray irradiation. Further, any suitable method may be used as a method of dispersing the particles in the resin for forming a cladding layer.

The SPR sensor cell and the colorimetric sensor cell of the present invention can be obtained by forming desired components (a protective layer, a metal layer, an over-cladding layer, and the like) on the core exposed surface of the optical waveguide of the present invention. Methods described in JP 2012-107901 A, JP 2012-215541 A, and the like can be used as methods of forming those components.

EXAMPLES

The present invention is hereinafter described specifically by way of Examples. However, the present invention is not limited to the Examples below.

The refractive index was measured by forming a film having a thickness of 10 μm on a silicon wafer and measuring the refractive index of the film at a wavelength of 830 nm through use of a prism coupler refractive index measurement device.

The filling ratio of the particles was calculated based on the following expression.

Filling ratio (%)=((particle mixing rate (wt %)/bulk specific gravity (g/mL))/(100+particle mixing rate (wt %)))×100

The bulk specific gravity of the particles was calculated by loading the particles into a cup having a known volume (mL), measuring a particle weight (g), and dividing the particle weight by the cup volume.

A median diameter calculated through the laser diffraction/scattering particle size distribution measurement was used as the average particle diameter.

Measurement was performed in accordance with the section 5.4 Scratch Hardness (Pencil Method) of JIS K 5600: Testing Methods for Paints.

DMA measurement was performed using a thermal analysis apparatus (manufactured by NETZSCH, product number: “DMA 242 C”). The measurement was performed under the conditions of a rate of temperature increase of 2° C./min and a measurement frequency of 1 Hz. A storage modulus at 25° C. was determined from the resultant DMA curve.

<Crack>

The presence or absence of a crack in the surface of an optical waveguide was visually observed.

Example 1

An SPR sensor cell was produced by a method illustrated in FIG. 6. Specifically, a material for forming a core layer was dropped onto the surface of a die (length: 200 mm, width: 200 mm) having formed on its surface a recessed portion for forming a core layer having a width of 50 μm and a length (depth) of 50 μm. One end of a corona-treated surface of a PP film (thickness: 40 μm) having one surface subjected to corona treatment was brought into abutment against the surface of the die, and the other end was allowed to be warped. In this state, a roller was rotated toward the other end side while pressing the abutment part between the die and the PP film from the PP film side, to thereby bond the die and the PP film to each other. With this, the material for forming a core layer was filled into the recessed portion of the die, and thus the excessive material for forming a core layer was pushed out. Then, the material for forming a core layer was completely cured by irradiating the laminate thus obtained with ultraviolet rays from the PP film side. Thus, a core layer (refractive index: 1.384) was formed. The material for forming a core layer was prepared by stirring and dissolving 60 parts by weight of a fluorine-based UV-curable resin (“OP38Z” (trade name) manufactured by DIC Corporation) and 40 parts by weight of a fluorine-based UV-curable resin (“OP4OZ” (trade name) manufactured by DIC Corporation). Then, the PP film was peeled from the die. Thus, the core layer having a substantially square column shape with a thickness of 50 μm and a width of 50 μm was transferred onto the film.

A material for forming a cladding layer was applied to the PP film so as to cover the core layer. The material for forming a cladding layer was prepared by mixing 99.4 parts by weight of a fluorine-based UV curable resin (“Fluorolink MD700” (trade name) manufactured by Solvay Specialty Polymers Japan K.K., refractive index: 1.348) and 0.6 part by weight of silica particles (“Admafine SC2500-SMJ” (trade name) manufactured by Admatechs Company Limited, refractive index: 1.45). At this time, the material for forming a cladding layer was applied so that the thickness from a surface (upper surface) of the core layer became 100 um. Then, the material for forming a cladding layer was cured by irradiating the resultant with ultraviolet rays. Thus, a cladding layer was formed. Then, the PP film was removed by peeling, and the cladding layer and the core layer were inverted. As described above, an optical waveguide film having a core layer buried in a cladding layer was produced.

Example 2

An optical waveguide film was produced in the same way as in Example 1 except that the mixing rate of the silica particles in the material for forming a cladding layer was set to 2.5 wt %.

Example 3

An optical waveguide film was produced in the same way as in Example 1 except that the mixing rate of the silica particles in the material for forming a cladding layer was set to 5 wt %.

Example 4

An optical waveguide film was produced in the same way as in Example 1 except that the mixing rate of the silica particles in the material for forming a cladding layer was set to 10 wt %.

Example 5

An optical waveguide film was produced in the same way as in Example 1 except that different silica particles (“Admafine SC5500-SMJ” (trade name) manufactured by Admatechs Company Limited) were used, and the mixing rate of the silica particles in the material for forming a cladding layer was set to 0.8 wt %.

Example 6

Example 7

Example 8

Example 9

An optical waveguide film was produced in the same way as in Example 1 except that different silica particles (“AEROSIL R974” (trade name) manufactured by Nippon Aerosil Co., Ltd., refractive index: 1.45) were used, and the mixing rate of the silica particles in the material for forming a cladding layer was set to 2.6 wt %.

Example 10

Example 11

An optical waveguide film was produced in the same way as in Example 1 except that different silica particles (“SYLOPHOBIC 507” (trade name) manufactured by Fuji Silysia Chemical Ltd., refractive index: 1.45) were used, and the mixing rate of the silica particles in the material for forming a cladding layer was set to 3.2 wt %.

Example 12

An optical waveguide film was produced in the same way as in Example 1 except that different silica particles (“SYLOPHOBIC 702” (trade name) manufactured by Fuji Silysia Chemical Ltd., refractive index: 1.45) were used, and the mixing rate of the silica particles in the material for forming a cladding layer was set to 4 wt %.

Example 13

Example 14

An optical waveguide film was produced in the same way as in Example 1 except that titania particles (“SRD 02-W” (trade name) manufactured by Sakai Chemical Industry Co. Ltd., crystal phase: rutile type, refractive index: 2.72) were used, and the mixing rate of the titania particles in the material for forming a cladding layer was set to 2 wt %.

Example 15

An optical waveguide film was produced in the same way as in Example 1 except that different silica particles (“Admafine SC1500-SMJ” (trade name) manufactured by Admatechs Company Limited, refractive index: 1.45) were used, and the mixing rate of the silica particles in the material for forming a cladding layer was set to 6.5 wt %.

Example 16

Comparative Example 1

An optical waveguide film was produced in the same way as in Example 1 except that the mixing rate of the silica particles in the material for forming a cladding layer was set to 0 wt % (that is, the silica particles were not used).

Comparative Example 2

An optical waveguide film was produced in the same way as in Example 1 except that the mixing rate of the silica particles in the material for forming a cladding layer was set to 0.3 wt %.

Comparative Example 3

An optical waveguide film was produced in the same way as in Example 1 except that the mixing rate of the silica particles in the material for forming a cladding layer was set to 26 wt %.

Comparative Example 4

The evaluation results of each of the optical waveguide films obtained in the Examples and Comparative Examples are shown in Table 1.

TABLE 1

Average

particle
Mixing
Filling

Storage

diameter
rate
ratio
Surface
modulus

(μm)
(wt %)
(%)
hardness
(GPa)
Crack

Example 1
0.5
0.6
2
2H
0.15
Absent

Example 2
0.5
2.5
8
2H
0.19
Absent

Example 3
0.5
5
14
H
0.19
Absent

Example 4
0.5
10
25
H
0.23
Absent

Example 5
1.9
0.8
2
2H
0.16
Absent

Example 6
1.9
2
5
2H
0.19
Absent

Example 7
1.9
5
11
HB
0.20
Absent

Example 8
1.9
10
20
H
0.21
Absent

Example 9
0.012
2.6
34
H
0.22
Absent

Example 10
0.012
5
50
2H
0.23
Absent

Example 11
2.7
3.2
8
2H
0.20
Absent

Example 12
4.1
4
12
H
0.23
Absent

Example 13
4.1
7.2
20
2H
0.25
Absent

Example 14
0.035
2
30
H
0.19
Absent

Example 15
0.3
6.5
14
2H
0.16
Absent

Example 16
0.3
10
30
HB
0.20
Absent

Comparative
—
—
0
4H
0.12
Present

Example 1

Comparative
0.5
0.3
1
3H
0.13
Present

Example 2

Comparative
0.5
26
60
3H
0.23
Present

Example 3

Comparative
4.1
25
70
5H
0.30
Present

Example 4

As is apparent from Table 1, in each of the optical waveguides of the Comparative Examples including a cladding layer having a surface hardness of more than 2H, a crack occurred in the cladding layer. On the other hand, in each of the optical waveguides of the Examples including a cladding layer having a surface hardness of 2H or less, the occurrence of a crack was prevented. In addition, according to the present invention, the occurrence of a crack can be prevented by adding particles to a resin which has heretofore been preferably selected from the viewpoints of optical properties, workability, and the like (such as a halogen-containing resin), and hence there is also an advantage in that it is not necessary to develop or select a new resin capable of preventing the occurrence of a crack.

INDUSTRIAL APPLICABILITY

The optical waveguide of the present invention can be suitably used as the detection unit of the SPR sensor cell, the colorimetric sensor cell, or the like.

REFERENCE CHARACTER LIST

11 cladding layer (under-cladding layer)

12 core layer

20 metal layer

30 over-cladding layer

40 protective layer

100 optical waveguide

200 SPR sensor cell

300 colorimetric sensor cell

Number	Date	Country	Kind
2013-245640	Nov 2013	JP	national
2014-176704	Sep 2014	JP	national

Optical Waveguide, and SPR Sensor Cell and Colorimetric Sensor Cell Which Use Optical Waveguide

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