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42 results about "Dipole mode" patented technology

Topological bulk laser based on energy band inversion light field limiting effect and method

The invention discloses a topological bulk laser based on an energy band inversion light field limiting effect and a method, being characterized in that a topological state photonic crystal which generates a dipole mode and a quadrupole mode near the center of a Brillouin zone and generates energy band reversing and a topological moderate state photonic crystal which does not generate energy bandreversing are adopted; the spliced boundary can generate reflection and limitation effects of a light field, and the boundary encircles to form a closed curve, so that a laser resonant cavity is formed in the boundary. According to the topological bulk laser based on an energy band inversion light field limiting effect and the method, single-mode vertical laser emission with high directivity, lowthreshold, narrow linewidth and high side-mode rejection ratio can be realized; the process difficulty and the preparation cost are reduced; the problems of heat dissipation and electric injection areimproved; the stability of components is improved, and the service life is prolonged; after copying to an electric injection active material system, the topological bulk laser based on an energy bandinversion light field limiting effect can obtain the vertical emitting laser with controllable size, high directivity, low threshold, narrow linewidth and high side mode rejection ratio; and the topological bulk laser based on an energy band inversion light field limiting effect can be applied to the fields of optical communication, solid-state lighting, laser radar, substance detection, medicaldiagnosis and the like.
Owner:PEKING UNIV

Polarizing reflector for multiple beam antennas

A polarizing reflector for broadband antennas includes a flat dielectric substrate, a patch array layer formed by a bi-dimensionally periodic lattice of thin metallic patches along first and second perpendicular directions x, y, and a ground layer. All the patches have a same shape elongated along the second direction y and form electric dipoles when electrically excited along the second direction y. For each row the patches of the said row are interconnected by an elongated metallic strip oriented along the first direction x and having a width c. The geometry of the patch array, the thickness h and the dielectric permittivity εr of the substrate, and the width c of the elongated metallic strips are tuned so that the patch array including the elongated metallic strips induces a fundamental aperture mode and a complementary fundamental dipolar mode along two orthogonal TE and TM polarizations within a single operating frequency band or two separate operating frequency bands, and the differential phase between the two fundamental modes over the single or the first and second frequency bands being equal to ±90° or to an odd integer multiple of ±90°. The polarizing reflector can comprise also a curved substrate and a patch array layer formed by a bi-dimensionally lattice of metallic patches along first curvilinear rows and second curvilinear columns.
Owner:THALES SA

Dielectric resonator based on equivalent localized surface plasmon polaritons and working method thereof

InactiveCN109755713AAchieving Multipole ResonanceInfinitely smallResonatorsEffective surfaceDielectric resonator antenna
The invention discloses a dielectric resonator based on equivalent local area type surface plasmon polaritons and a working method thereof. The dielectric resonator comprises a dielectric column, a metal patch and metal wires, the metal wires are periodically arranged along the side surface of the dielectric column, the metal patch is attached to the upper and bottom surfaces of the dielectric column and is connected with the metal wires. The main mode of the dielectric resonator is an electric dipole mode of the effective surface plasmon polariton, when the electromagnetic wave is incident onthe resonator at a certain frequency, the effective localized surface plasmon polaritons can be generated on a junction surface of the dielectric column and the external air under the induction of the metal wires, so that effective localized surface plasma resonance is generated. The resonant frequency of the main mode of the dielectric resonator in the invention changes along with the change ofthe height of the resonator and the dielectric constant of the medium, but the resonant frequency of the main mode is not sensitive to the change of the diameter of the resonator. Therefore, the volume of the dielectric resonator in the invention can be multiple times smaller than that of the traditional dielectric resonator.
Owner:NANJING UNIV OF AERONAUTICS & ASTRONAUTICS

Polarizing reflector for multiple beam antennas

A polarizing reflector for broadband antennas includes a flat dielectric substrate, a patch array layer formed by a bi-dimensionally periodic lattice of thin metallic patches along first and second perpendicular directions x, y, and a ground layer. All the patches have a same shape elongated along the second direction y and form electric dipoles when electrically excited along the second direction y. For each row the patches of the said row are interconnected by an elongated metallic strip oriented along the first direction x and having a width c. The geometry of the patch array, the thickness h and the dielectric permittivity εr of the substrate, and the width c of the elongated metallic strips are tuned so that the patch array including the elongated metallic strips induces a fundamental aperture mode and a complementary fundamental dipolar mode along two orthogonal TE and TM polarizations within a single operating frequency band or two separate operating frequency bands, and the differential phase between the two fundamental modes over the single or the first and second frequency bands being equal to +90° or to an odd integer multiple of ±90°. The polarizing reflector can comprise also a curved substrate and a patch array layer formed by a bi-dimensionally lattice of metallic patches along first curvilinear rows and second curvilinear columns.
Owner:THALES SA

Refractive index sensor based on asymmetric nanostructure perfect absorber, sensing test device and method

PendingCN114166799ARealize detectionSolve the limitation that it is difficult to break through the diffraction limitPhase-affecting property measurementsRefractive indexGold film
The invention provides a refractive index sensor based on an asymmetric nanostructure perfect absorber, a sensing test device and a sensing test method. The refractive index sensor comprises a substrate, a gold film, a spacing layer and a nanometer meniscus array, the gold film is evaporated on the substrate and is used for eliminating transmission; the spacing layer is arranged on the gold film and is used for spacing the gold film and the nano meniscus array; the nanometer meniscus array is arranged on the spacing layer, and when light irradiation and the nanometer meniscus array resonate, a local surface plasmon resonance dipole mode or a high-order mode is excited. According to the invention, by controlling and changing the polarization of incident light, different high-order local surface plasmon resonance modes are selectively excited by using the asymmetric nanometer meniscus perfect absorber, and the high-order plasmon resonance modes have relatively small radiation; and due to the perfect absorption property, the refractive index sensor utilizes inevitable loss in daily life, and transmission is reduced, so that the refractive index sensor has relatively high absorption, and the purposes of obtaining a narrow-band spectrum and improving the detection sensitivity of the sensing device are achieved.
Owner:DALIAN MARITIME UNIVERSITY

Perfect circular polarization separator based on magnetoelectric coupling

PendingCN113777794AAchieve perfect circular polarization separationLow costOptical elementsCircular discRotational axis
The invention provides a perfect circular polarization separator based on magnetoelectric coupling. The separator is composed of a ceramic disc and a central air hole, the rotating axis of the ceramic disc and the rotating axis of the central air hole coincide, and the central air hole cannot penetrate through the ceramic disc, so that magnetoelectric coupling of the structure is realized, incident light is linear polarization planar light, and the propagation direction is perpendicular to the rotating axis of the structure. The polarization direction of the linear polarization plane light is parallel or perpendicular to the rotating axis of the structure. The ceramic material is adopted as a basic material, and the advantage of low cost is achieved; a complicated light source device for realizing perfect circular polarization separation in the past is simplified by plane light incidence; and the magnetoelectric coupling characteristic of the composite structure of the ceramic disc and the central air hole is beneficial to excitation of a longitudinal dipole mode which is difficult to excite by a common structure, so that a transverse spin dipole moment is constructed, and perfect separation of left-handed and right-handed circular polarization can be effectively realized.
Owner:HARBIN ENG UNIV

Graphene-based light operation-control system and light operation-control method

The invention discloses a graphene-based light operation-control system. The system comprises a target particle at a target position and a wave beam generating apparatus; the target particle is a core-shell structure, and comprises core-layer graphene and shell-layer graphene; and the wave beam generating apparatus is used for generating a first-order Bessel wave beam to illuminate the target particle, so that respective electric dipole modes of the core-layer graphene and the shell-layer graphene are coupled with respective electric quadrupole modes to form Fano resonances, a light pulling force directed to the wave beam generating apparatus is applied to the target particle, and the target particle is moved to the wave beam generating apparatus. By illumination of the first-order Besselwave beam, forward scattering can be promoted while backward scattering can be suppressed, so that a relatively large negative optical force is obtained, movement of the target particle by pulling thetarget particle along a direction of the wave beam generating apparatus is realized, a distance between the target particle and the wave beam generating apparatus is shortened, and thereby movement of the target particle is realized. The invention also provides a light operation-control method which has the above beneficial effects.
Owner:SUZHOU UNIV

A graphene-based light manipulation system and light manipulation method

The invention discloses a graphene-based light operation-control system. The system comprises a target particle at a target position and a wave beam generating apparatus; the target particle is a core-shell structure, and comprises core-layer graphene and shell-layer graphene; and the wave beam generating apparatus is used for generating a first-order Bessel wave beam to illuminate the target particle, so that respective electric dipole modes of the core-layer graphene and the shell-layer graphene are coupled with respective electric quadrupole modes to form Fano resonances, a light pulling force directed to the wave beam generating apparatus is applied to the target particle, and the target particle is moved to the wave beam generating apparatus. By illumination of the first-order Besselwave beam, forward scattering can be promoted while backward scattering can be suppressed, so that a relatively large negative optical force is obtained, movement of the target particle by pulling thetarget particle along a direction of the wave beam generating apparatus is realized, a distance between the target particle and the wave beam generating apparatus is shortened, and thereby movement of the target particle is realized. The invention also provides a light operation-control method which has the above beneficial effects.
Owner:SUZHOU UNIV
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