A spatial filtering apparatus includes a composite filter including first filter patterns respectively having a first phase profile, and second filter patterns respectively having a second phase profile, wherein the first filter patterns and the second filter patterns overlap with each other, wherein first light in a first polarization direction that is emitted on the composite filter is first spatially filtered by the first filter patterns, and wherein second light in a second polarization direction that is emitted on the composite filter is second spatially filtered by the second filter patterns.

Various embodiments may provide an optical sensing device based on surface plasmon resonance (SPR). The optical sensing device may include an optical arrangement configured to provide a first polarization light beam and a second polarization light beam, and a first optical member including a sensing surface, the first optical member configured to receive the first and second polarization light beams and reflect the first and second polarization light beams at the sensing surface. The optical sensing device may further include a second optical member arranged to receive the reflected first and second polarization light beams from the first optical member and configured to separate the reflected first and second polarization light beams in a first direction and a second direction, respectively. The optical device may additionally include a detector arrangement configured to detect the reflected first and second polarization light beams from the second optical member.

A transition metal dichalcogenides device includes a substrate, at least one layer of boron nitride, a tungsten diselenide monolayer positioned such that the at least one layer of boron nitride at least partially encapsulates the tungsten diselenide monolayer, and a plurality of electrodes. Each of the plurality of electrodes includes gold and few-layer graphene, and the at least one layer of boron nitride includes hexagonal few-layer boron nitride. The tungsten diselenide monolayer is configured to reveal excitons when at least one of a K valley and a K valley of the tungsten diselenide monolayer is exposed to excitation photon energy and an external magnetic field. The excitons are giant valley-polarized Rydberg excitons in excited states ranging from 2 s to 11 s when the external magnetic field is in the range of about ?17 T to about 17 T.

A transition metal dichalcogenides device includes a substrate, at least one layer of boron nitride, a tungsten diselenide monolayer positioned such that the at least one layer of boron nitride at least partially encapsulates the tungsten diselenide monolayer, and a plurality of electrodes. Each of the plurality of electrodes includes gold and few-layer graphene, and the at least one layer of boron nitride includes hexagonal few-layer boron nitride. The tungsten diselenide monolayer is configured to reveal excitons when at least one of a K valley and a K valley of the tungsten diselenide monolayer is exposed to excitation photon energy and an external magnetic field. The excitons are giant valley-polarized Rydberg excitons in excited states ranging from 2 s to 11 s when the external magnetic field is in the range of about ?17 T to about 17 T.

An illumination device 11 has: a light source 1 for emitting polarized light having a Gaussian beam profile and including a first polarized light component and a second polarized light component orthogonal to each other; and a spiral phase element for imparting a phase modulation amount which increases for each predetermined step amount along a circumferential direction about an optical axis OA to the first polarized light component of transmitted polarized light from the light source 1 and making the beam profile of the first polarized light component a Laguerre-Gaussian beam profile, and forming a composite beam having a top-hat-shaped beam profile in which the second polarized light component of the transmitted polarized light from the light source 1 and the first polarized light component having a Laguerre-Gaussian beam profile are synthesized.

In ellipsometer and polarimeter systems, reflective optics including both convex and a concave mirrors that have beam reflecting surfaces, as well as aperture control of beam size to optimize operation with respect to aberration and diffraction effects while achieve the focusing of a beam of electromagnetic radiation with minimized effects on a polarization state of an input beam state of polarization that results from adjustment of angles of incidence and reflections from the various mirrors involved, and further including detectors of electromagnetic radiation that enable optimization of the operation thereof for application over various specific wavelength ranges, involving functional combinations of gratings and/or combination dichroic beam splitter-prisms, which themselves can be optimized as regards wavelength dispersion characteristics.

In ellipsometer and polarimeter systems, reflective optics including both convex and a concave mirrors that have beam reflecting surfaces, as well as aperture control of beam size to optimize operation with respect to aberration and diffraction effects while achieve the focusing of a beam of electromagnetic radiation with minimized effects on a polarization state of an input beam state of polarization that results from adjustment of angles of incidence and reflections from the various mirrors involved, and further including detectors of electromagnetic radiation that enable optimization of the operation thereof for application over various specific wavelength ranges, involving functional combinations of gratings and/or combination dichroic beam splitter-prisms, which themselves can be optimized as regards wavelength dispersion characteristics.

A rain sensor is included in a vehicle, and a method for controlling the vehicle utilizes the rain sensor. The rain sensor includes a light transmitter configured to radiate light to a windshield of the vehicle; a light receiver configured to receive light reflected from the windshield to generate a reception light signal; a filter configured to filter out noise from the reception light signal; and a controller configured to determine a presence or absence of pollutant and a degree of pollution on the basis of the filtered reception light signal, and perform pollutant removing.

The present invention provides an ellipsometry device and an ellipsometry method whereby measurement efficiency can be enhanced. In this method, an object is illuminated by spherical-wave-like illumination light Q linearly polarized at 45 (S1), and an object light O, being a reflected light, is acquired in a hologram I.sub.OR using a spherical-wave-like reference light R having a condensing point near the condensing point of the illumination light Q, and a hologram I.sub.LR of the reference light R is furthermore acquired using a spherical-wave reference light L having the same condensing point as that of the illumination light Q (S2). The holograms are separated into p- and s-polarized light holograms I.sup.K.sub.OR, I.sup.K.sub.LR, =p, s and processed to extract object light waves, and object light spatial frequency spectra G.sup.K(u, v), =p, s are generated (S3) (S4). Ellipsometric angles (), () are obtained for each incident angle from the amplitude reflection coefficient ratio =G.sup.p/G.sup.s=tan .Math.exp(i). Through use of numerous lights having different incident angles included in the illumination light Q, data of numerous reflection lights can be acquired collectively in a hologram and can be processed.

The present invention provides an ellipsometry device and an ellipsometry method whereby measurement efficiency can be enhanced. In this method, an object is illuminated by spherical-wave-like illumination light Q linearly polarized at 45 (S1), and an object light O, being a reflected light, is acquired in a hologram I.sub.OR using a spherical-wave-like reference light R having a condensing point near the condensing point of the illumination light Q, and a hologram I.sub.LR of the reference light R is furthermore acquired using a spherical-wave reference light L having the same condensing point as that of the illumination light Q (S2). The holograms are separated into p- and s-polarized light holograms I.sup.K.sub.OR, I.sup.K.sub.LR, =p, s and processed to extract object light waves, and object light spatial frequency spectra G.sup.K(u, v), =p, s are generated (S3) (S4). Ellipsometric angles (), () are obtained for each incident angle from the amplitude reflection coefficient ratio =G.sup.p/G.sup.s=tan .Math.exp(i). Through use of numerous lights having different incident angles included in the illumination light Q, data of numerous reflection lights can be acquired collectively in a hologram and can be processed.