Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/97830
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dc.contributorDepartment of Electronic and Information Engineering-
dc.creatorYuan, J-
dc.creatorZhang, J-
dc.creatorChen, MK-
dc.creatorTsai, DP-
dc.date.accessioned2023-03-23T03:33:12Z-
dc.date.available2023-03-23T03:33:12Z-
dc.identifier.urihttp://hdl.handle.net/10397/97830-
dc.language.isozhen_US
dc.publisher中华人民共和国国家知识产权局en_US
dc.rightsAssignee: 香港理工大学深圳研究院en_US
dc.titleTotal space focus adjustable super-structure lens and design method thereofen_US
dc.typePatenten_US
dc.description.otherinformationInventor name used in this publication: 袁家琪en_US
dc.description.otherinformationInventor name used in this publication: 张景程en_US
dc.description.otherinformationInventor name used in this publication: 陈沐谷en_US
dc.description.otherinformationInventor name used in this publication: 蔡定平en_US
dc.description.otherinformationTitle in Traditional Chinese: 一種全空間焦點可調超構透鏡及其設計方法en_US
dcterms.abstractThe invention discloses a total-space focus-adjustable super-structure lens and a design method thereof, the total-space focus-adjustable super-structure lens comprises a first super-structure surface, a second super-structure surface and a third super-structure surface, and emergent wave phases corresponding to nano antennas of the first super-structure surface meet a formula: P1 =-a ((x1 + d) 2 + y12), the emergent wave phase corresponding to each nano antenna on the second metasurface meets the formula: P2 = a ((x2 + d) 2 + y22) (a (x22 + y22)) phi 1, the emergent wave phase corresponding to each nano antenna on the third metasurface meets the formula: P3 =-(a (x32 + y32)) phi 2, a and d are constants, x1 and y1 are first plane coordinates corresponding to each nano antenna on the first metasurface, x2 and y 2 are second plane coordinates corresponding to the nano antennas on the second metasurface, x3 and y3 are third plane coordinates corresponding to the nano antennas on the third metasurface, phi < 1 > and phi < 2 > are angles under a cylindrical coordinate system, phi < 1 > = tan-1 (y2/x2), and phi < 2 > = tan-1 (y3/x3). The planar structure of the super-structure lens avoids spherical aberration and chromatic aberration, the numerical aperture is increased, the super-structure lens is small in size and beneficial to integration, and free adjustment of the full-space focus can be achieved.-
dcterms.abstract本发明公开了一种全空间焦点可调超构透镜及其设计方法,包括:第一超构表面、第二超构表面以及第三超构表面,第一超构表面的各个纳米天线对应的出射波相位满足公式:P1=‑a((x1+d)2+y12),第二超构表面的各个纳米天线对应的出射波相位满足公式:P2=a((x2+d)2+y22)(a(x22+y22))φ1,第三超构表面的各个纳米天线对应的出射波相位满足公式:P3=‑(a(x32+y32))φ2,其中,a和d为常数,x1和y1为第一超构表面的各个纳米天线对应的第一平面坐标,x2和y2为第二超构表面的各个纳米天线对应的第二平面坐标,x3和y3为第三超构表面的各个纳米天线对应的第三平面坐标,φ1和φ2为柱坐标系下的角度,φ1=tan‑1(y2/x2),φ2=tan‑1(y3/x3)。本发明的超构透镜的平面化结构避免了球差、色差的产生,增加了数值孔径,超构透镜体积小,利于集成,可实现全空间焦点自由可调。-
dcterms.accessRightsopen accessen_US
dcterms.alternative一种全空间焦点可调超构透镜及其设计方法-
dcterms.bibliographicCitation中国专利 ZL202110456064.2-
dcterms.issued2022-09-09-
dc.description.countryChina-
dc.description.validate202303 bcch-
dc.description.oaVersion of Recorden_US
dc.description.pubStatusPublisheden_US
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