Abstract: A Raman spectroscopic device includes an optical resonator, in which a first reflecting body that exhibits semi transmissivity/semi reflectivity and has a surface which is a light scattering surface that generates Raman scattering, a transparent body, and a second reflecting body that exhibits reflectivity, are laminated in sequence one on another. The Raman spectroscopic device utilizes light absorption due to resonance to obtain a surface amplified Raman effect.

Abstract: An organic electroluminescence device having two electrodes and a plurality of organic layers between the two electrodes, in which the organic layers include a light emitting layer that emits light when an electric field is applied between the two electrodes. The device further includes, inside or on the organic layer side of at least either one of the electrodes, a metal structure that generates a surface or local plasmon by light emitted from the light emitting layer, and the metal structure is embedded in a conductive layer and at least a portion of the metal structure is located adjacent to the light emitting layer.

Abstract: A microstructure is formed on a conductor. The microstructure is equipped with a dielectric base material, in which a great number of fine holes having substantially the same shape in plan view are formed. The fine holes are open at the surface of the dielectric base material, and are substantially uniformly provided therein. A plurality of micro metal members are fixed to the dielectric base material. The micro metal members include filling portions that fill one or more of the fine holes, and protruding portions that protrude from the surface of the dielectric base material and are of diameters greater than the fine holes, capable of inducing local plasmon. The plurality of micro metal members include those that have different numbers of filling portions.

Abstract: The present invention provides a heat ray-shielding material which includes metal particle-containing layer containing at least one kind of metal particle, wherein the metal particle contains substantially hexagonal or substantially discoidal metallic flat particles in an amount of 60% by number or more, and the main planes of the metallic flat particles are oriented at an angle ranging from 0° to ±30° relative to one surface of the metal particle-containing layer.

Abstract: A sensor has a sensing surface, to which a specific substance R to be detected can bind. Further, the sensor has a metal portion, at least a portion of which is exposed at the sensing surface, and in which localized plasmons can be excited. The sensor is used in sensing, in which the substance R to be detected is marked with a fluorescent marker Lu that selectively binds to the substance R to be detected and one of two-photon excitation fluorescence and multi-photon excitation fluorescence of the fluorescent marker Lu is detected. Further, the sensing surface is illuminated with measurement light L1 having a wavelength that can excite localized plasmons in the metal portion and that is an absorption wavelength of the fluorescent marker Lu, at which the fluorescent marker Lu emits one of the two-photon excitation fluorescence and the multi-photon excitation fluorescence.

Abstract: A sensing system using a sensing element being constituted by a transparent body sandwiched by first and second reflectors one or each of which is in contact with a specimen, and exhibiting an absorption characteristic varying with the specimen. The first reflector is a partially transparent reflective, and the second reflector is completely reflective, or partially transparent reflective. A light injection unit injects light onto the first reflector, and a light detection unit detects the intensity of light outputted from the sensing element in response to the injection. The light injection unit has a wavelength stabilizing arrangement and injects laser light, or injects light at two wavelengths. In the latter case, the light detection unit detects the intensities of outputted light at the two wavelengths, and a calculation unit obtains the difference between the intensities.

Abstract: A measurement apparatus includes a dielectric block, a thin film layer formed on the dielectric block and brought into contact with a sample, a light source for generating a light beam, an optical incident system for causing the light beam to enter the dielectric block so that the light beam is totally reflected at the interface between the dielectric block and the thin film, and a two-dimensional light detection means for detecting the intensity of the light beam totally reflected at the interface. A predetermined pattern is formed within a region irradiated with the light beam on the dielectric block. The measurement apparatus includes a correction means for correcting an output from the two-dimensional light detection means, based on the pattern, so that an object on the face of the dielectric block is similar to the object detected by the two-dimensional detection means.

Abstract: A surface plasmon resonance measuring apparatus is provided with a dielectric block, a metal film formed on a surface of the dielectric block, a light source for emitting a light beam, an optical system for making the light beam enter the dielectric block at various angles of incidence so that a condition for total internal reflection is satisfied at an interface between the dielectric block and the thin film layer, and a photodetector for detecting the intensity of the light beam satisfying total internal reflection at the interface. In the measurement chip to be utilized in the surface plasmon resonance measuring apparatus, the dielectric block is formed from a synthetic resin in which, when said light beam is p-polarized outside said dielectric block and then strikes the interface, the intensity of a s-polarized component at the interface is 50% or less of the intensity of the light beam at the interface.

Abstract: A Raman spectroscopic device includes an optical resonator, in which a first reflecting body that exhibits semi transmissivity/semi reflectivity and has a surface which is a light scattering surface that generates Raman scattering, a transparent body, and a second reflecting body that exhibits reflectivity, are laminated in sequence one on another. The Raman spectroscopic device utilizes light absorption due to resonance to obtain a surface amplified Raman effect.

Abstract: An imaging apparatus includes a solid state imaging device having a light receiving characteristic in which an amount of light received reaches a maximum when an angle of incidence of parallel light, radiated at continuously changing angle, is not vertical (angle ? of incident light in the range of 3° to 15°) to a light receiving surface. This characteristic changes the amount of light received greatly when an aperture stop is opened, and enhances an opening/closing effect of the aperture stop. The solid state imaging device includes a core/clad light guide path structure, whose core serves as a light guide path. This light guide path includes a columnar portion located above a photodiode, and a lens portion on the columnar portion.

Abstract: A mass spectroscopy device constituted by a first reflector which is partially transparent and partially reflective, a transparent body, and a second reflector which is reflective. The first reflector and the second reflector are arranged on opposite sides of the transparent body so as to form an optical resonator in such a manner that when a specimen containing an analyte subject to mass spectroscopy is arranged in contact with a surface of the first reflector, and the surface is irradiated with measurement light, optical resonance occurs in the optical resonator, and intensifies an electric field on the surface, and the intensified electric field desorbs the analyte from the surface.

Abstract: A photoelectric converting device comprises: a first electrode layer having conductivity; a metal filled dielectric layer formed on said first electrode layer and comprising a dielectric base material in which a plurality of micropores are formed, and a plurality of conductive fine metal bodies made of a metal material which fills said plurality of micropores formed in said dielectric base material; a photoelectric converting layer that is formed on said metal filled dielectric layer and is made of a photoelectric converting material; and a second electrode layer having conductivity that is formed on said photoelectric converting layer; each of said fine metal bodies including a protruding unit that protrudes from said dielectric base material to within said photoelectric converting layer, and being electrically connected to said first electrode layer; said photoelectric converting layer covering said protruding unit of each of said fine metal bodies.

Abstract: A new and novel sensor having a simple structure with high detection sensitivity. The sensor (S1) includes the following from measuring light (L1) input side in the order listed below: a first reflector (10) having semi-transmissive and semi-reflective properties; a translucent body (20); and a second reflector (30) having perfect reflection properties, or semi-transmissive and semi-reflective properties. The first reflector (10) and/or second reflector is brought into contact with a specimen, and the average complex refractive index varies with the specimen. Absorption properties for absorbing light having a particular wavelength are produced by these components, the properties of the measuring light (L1) are changed by the optical properties including the absorption properties, the output light (L2) is outputted from the first reflector (10) and/or second reflector (30), and the physical properties of the output light (L2) that vary according to the optical properties are detected.

Abstract: A Raman spectrum detecting method includes a liquid sample contacting step of placing a liquid sample containing a reference substance and a specimen in contact with a detection surface, the reference substance generating a known Raman spectrum having at least one peak therein that is different from peaks in a Raman spectrum generated by the specimen; a scattered light detecting step of irradiating the detection surface in contact with the liquid sample with an excitation light and detecting Raman scattered light occurring from the liquid sample; and a normalizing step of extracting a Raman spectrum signal of the reference substance and a Raman spectrum signal of the specimen from the signal detected in the scattered light detecting step and normalizing a signal intensity of the Raman spectrum signal of the specimen according to an intensity of the Raman spectrum signal of the reference substance.

Abstract: A sensor is an optical resonator constituted by: a first reflecting body that exhibits semi transmissivity/semi reflectivity; a transparent body; and a second reflecting body that exhibits one of reflectivity and semi transmissivity/semi reflectivity, provided in this order from the light incident side. The sensor is configured such that the absorption peak of the measuring light beam by resonance in the optical resonator matches the absorption peak of the measuring light beam by local plasmon resonance generated at the surface and/or within the optical resonator. The sensor has absorption properties such that light of specific wavelengths are absorbed depending the mean complex refractive indices of the first and second reflecting bodies and the thickness of the transparent body. An emitted light beam is output from the first reflecting body. The physical properties of the emitted light beam that change according to the absorption properties are detected.

Abstract: A near-field light-emitting element includes a transparent medium having a plane of incidence into which a laser beam enters, and a light-condensing plane on which the laser beam having entered the plane of incidence is concentrated, and a metal body provided on the light-condensing plane of the transparent medium having a first surface contacting the light-condensing plane, a second surface opposing the first surface, and an aperture which is formed to penetrate through the first and second surfaces at a position where the laser beam is concentrated and which emits a near-field light obtained from the laser beam. The metal body is arranged apart from a center of the aperture by a predetermined distance to connect together the first and second surfaces, and has a plasmon reflection plane that reflects toward the aperture a surface plasmon excited on the first and second surfaces by the laser beam concentrated at the aperture.

Abstract: A method of measuring Raman signals comprises: an analyte placing step of placing an analyte on a detection surface of a microstructure plate which generates an enhanced electric field when irradiated with excitation light; an irradiating step of irradiating the detection surface with the excitation light so that the enhanced electric field is generated around the detection surface and light is emitted from the analyte and the detection surface to be enhanced by the generated enhanced electric field; a Raman signal obtaining step of detecting the enhanced light to obtain a Raman signal emitted from the analyte and a background signal for use as a reference, the Raman signal and the background signal having respective intensities; and a normalizing step of normalizing the Raman signal from the analyte by dividing the intensity of the Raman signal from the analyte by the intensity of the background signal obtained as the reference.

Abstract: A mass spectroscope includes a mass analysis device having a surface provided with metallic members capable of exciting plasmons when irradiated by laser light, the mass analysis device allowing an analyte to be attached to the surface, a light radiation unit for irradiating the surface of the mass analysis device with laser light to ionize the analyte attached to the surface and desorb the analyte from the surface, and a detection unit for detecting a mass of the analyte ionized and desorbed from the surface of the mass analysis device from a time of flight of the analyte. The light radiation unit includes a polarization adjusting mechanism for adjusting a polarization direction of the laser light.

Abstract: A sensing system using a sensing element being constituted by a transparent body sandwiched by first and second reflectors one or each of which is in contact with a specimen, and exhibiting an absorption characteristic varying with the specimen. The first reflector is a partially transparent reflective, and the second reflector is completely reflective, or partially transparent reflective. A light injection unit injects light onto the first reflector, and a light detection unit detects the intensity of light outputted from the sensing element in response to the injection. The light injection unit has a wavelength stabilizing arrangement and injects laser light, or injects light at two wavelengths. In the latter case, the light detection unit detects the intensities of outputted light at the two wavelengths, and a calculation unit obtains the difference between the intensities.

Abstract: A new and novel sensor having a simple structure with high detection sensitivity. The sensor (S1) includes the following from measuring light (L1) input side in the order listed below: a first reflector (10) having semi-transmissive and semi-reflective properties; a translucent body (20); and a second reflector (30) having perfect reflection properties, or semi-transmissive and semi-reflective properties. The first reflector (10) and/or second reflector is brought into contact with a specimen, and the average complex refractive index varies with the specimen. Absorption properties for absorbing light having a particular wavelength are produced by these components, the properties of the measuring light (L1) are changed by the optical properties including the absorption properties, the output light (L2) is outputted from the first reflector (10) and/or second reflector (30), and the physical properties of the output light (L2) that vary according to the optical properties are detected.