A diffractometric sensor (1), comprises:a substrate (3);two interdigitated affinity gratings (2), a first affinity grating (20) comprising first unit cells (200) with affinity elements (201) and a second affinity grating (21) comprising second unit cells (210) with affinity elements (211), wherein the first unit cells (200) and second unit cells (210) are configured and arranged such that coherent light of a predetermined wavelength generated at a predetermined beam generation location (40) and diffracted by target molecules (204, 214)) bound to the affinity elements (201, 211) constructively interferes at a predetermined detection location (50) with an inverse phase, and wherein the first and second affinity gratings (20, 21) are balanced to generate a bias signal at the predetermined detection location (50) that corresponds to a difference (Am) in the scattering mass of the first and second affinity gratings (20, 21) which is in the range of 0.001 pg/mm.sup.2 to 30000 pg/mm.sup.2.

There is provided a chirped diffractive element (20) in the form of a grating (22) configured for supporting a plurality of guided mode resonances (54), which resonances (54) may be considered to comprise a standing wave. Chirping the grating (22) may allow guided mode resonances (54) to be distinguishable in terms of position within a section (34) the grating (22). An incident electromagnetic field may be coupled into at least one of the sections (34) when the electromagnetic field has a wavelength value within a predetermined wavelength range and a sample has a refractive index value within a predetermined index range. The incident electromagnetic field may be reflected by at least one of the sections (34) of the grating (22) exhibiting a guided mode resonance (54). The reflected electromagnetic field from the section (34) can then be detected by directly imaging the grating (22), thereby revealing the position of the exhibited guided mode resonance (54) in the grating (22), and thereby inferring the refractive index value of the sample.

The invention relates to a device (1) for detecting the presence of determined molecules, comprising, one on top of the other: a first substrate layer (11), a second reflection layer (12), and a third dielectric layer (13). The invention is characterised by an antenna array (14) with conductive parts (143), repeating in one direction (D, D2), the network (14) forming a plasmonic resonator (140) that can be brought into contact with the molecules and arranged so as to emit at least one thermal radiation peak corresponding to at least one characteristic mode of thermal vibration of the determined molecules.

A resin impregnation detection device configured to detect resin impregnation in a resin impregnation process for a coil insulation layer. The resin impregnation detection device can be inserted in a narrow portion, is capable of detecting impregnation with a liquid resin, and does not leave metal foreign materials other than an optical fiber in a product even after the resin impregnation. The resin impregnation detection device includes an optical fiber including an FBG sensor, and a coating resin, which coats the FBG sensor. The coating resin includes a resin to be softened by contact with a detection target resin. The FBG sensor is applied with a compressive strain caused by cure shrinkage of the coating resin or heat shrinkage thereof from a curing temperature to a normal temperature.

A target substance capturing device includes a reflection surface on which a plurality of non-flat portions is arrayed, the reflection surface capturing a target substance, and reflecting irradiated light. The plurality of non-flat portions are arranged in an array, the array includes a plurality of unit arrays in which the plurality of non-flat portions are arranged such that each one center of the non-flat portions superposes a position of a vertex in an M-time symmetrical figure, and the plurality of unit arrays is arranged such that each one center of gravity of the M-time symmetrical figure superposes a position of an intersection of an N-time symmetrical lattice pattern, where M is an integer of two or more, and N is an integer of two or more and different from M.

Disclosed is a resonant wavelength measurement apparatus, including a light source and a measurement unit. The measurement unit has a guided-mode resonance filter and a photosensitive element. The guided-mode resonance filter has a plurality of resonant areas, and each resonant area has a different filtering characteristic, to receive first light in the light source transmitted by a sensor or receive second light in the light source reflected by the sensor. The first light has a first corresponding pixel on the photosensitive element, the second light has a second corresponding pixel on the photosensitive element, and the first corresponding pixel and the second corresponding pixel correspond to a same resonant wavelength.

A fluorescence immunoassay device based on integration of a photonic crystal and magnetic beads and a method thereof are provided. Magnetic beads with high surface-to-volume ratio are used as carriers of fluorescent molecules to obtain higher fluorescence density. The electric field on the surface of the photonic crystal is enhanced through excitation of photonic crystal resonance. The intensity of the fluorescence signal excited by the enhanced electric field is increased. Moreover, through interaction with the photonic crystal, some fluorescent signals that originally cannot be received by the fluorescent sensor are coupled to the photonic crystal resonant modes and reradiate toward the fluorescent sensor, thereby increasing collection efficiency. The fluorescence signals generated by fluorescent molecules on the magnetic beads are significantly intensified, which could lower the detection limit. Furthermore, the magnetic beads aggregation method can achieve the detection capability that cannot be achieved by the current fluorescent immunoassay.

The application relates to methods of analyzing luminescent species. A substrate is provided that has a plurality of zero mode waveguides having apertures that extend through an upper non-reflective layer that is disposed on a lower transparent layer of a substrate. The apertures have non-reflective oxide layers on the reflective side walls of the apertures, the side walls having a thickness of greater than 10 nm, and the oxide layer is formed by oxidizing the non-reflective layer. The volume within the oxide layer defines a solution volume, and the volume within the reflective walls defines a ZMW volume. Having such non-reflective layers on the walls of the ZMW usefully decouples the solution volume from the ZMW volume.

The invention relates to an optical device (110) and a corresponding detection apparatus (100) that may for example be used for monitoring the replication of nucleotide sequences at a surface. In a preferred embodiment, the optical device (110) comprises a waveguide substrate (130) with a wiregrid (140) on a bottom surface (132), wherein apertures (141) of the wiregrid are in at least one direction (x) smaller than a characteristic wavelength () of input light (IL). Moreover, a diffractive structure (120) is disposed on the opposite surface (131) of the substrate (130) for coupling input light (IL) into the substrate (130) such that constructive interference occurs at the apertures (141). Thus evanescent waves can be generated with high efficiency in these apertures, allowing for example for a surface-specific excitation of fluorescence (FL) that can be sensed by a detector (160).

An optical sensing platform with an array of sensors, a laser or broadband light source and an optical detector that utilizes surface plasmon resonance based transduction and optical detection is provided. The sensor structure of the platform has a low index support layer, a high contrast grating, a low index spacer and a thin metal film with a target recognition element. The surface plasmon resonance based sensor uses surface plasmon waves to detect changes on the surface of the sensor when a target interacts with the target recognition element. The binding of the target with a recognition element receptor will induce changes in the refractive index of the metal layer, which changes the resonance wavelength of the plasmon wave on the sensor surface, which is used to measure or observe the reaction.