Author Affiliations
Abstract
State Key Laboratory of Precision Measurements Technology and Instruments, Department of Precision Instrument, Tsinghua University, Beijing 100084, China
Freeform surfaces are difficult to manufacture due to their lack of rotational symmetry. To reduce the requirements for manufacturing precision, a design method is proposed for freeform reflective-imaging systems with low surface-figure-error sensitivity. The method considers both the surface-figure-error sensitivity and optical specifications, which can design initial systems insensitive to surface figure errors. Design starts with an initial planar system; the surface-figure-error sensitivity of the system is reduced during construction. The proposed method and another that is irrelevant to figure-error sensitivity are used to design a freeform off-axis three-mirror imaging system. Comparison of the sensitivities of the two systems indicates the superiority of our proposed method.
220.4830 Systems design 080.4228 Nonspherical mirror surfaces 220.4610 Optical fabrication 080.4035 Mirror system design 
Chinese Optics Letters
2019, 17(9): 092201
Author Affiliations
Abstract
1 School of Optometry and Ophthalmology, Wenzhou Medical University, Wenzhou 325027, China
2 The Eye Hospital of Wenzhou Medical University, Wenzhou 325027, China
Astigmatism is inevitable and inherent to progressive addition lenses (PALs), which are typically distributed in the lateral areas on both sides of the progressive corridor. In this study, we took into account the spectacle frame for the customized freeform PAL design with the variational-difference numerical approach. The PAL surface with minimized astigmatism, approximately equal to 84% of the added power, was numerically resolved without expending the zone for clear vision. We validated our approach by experimentally demonstrating the procedure from tool path generation to surface power measurement, thus providing an efficient solution to the personalization of astigmatism-minimized PAL design and manufacture.
330.4460 Ophthalmic optics and devices 080.4225 Nonspherical lens design 
Chinese Optics Letters
2018, 16(11): 113302
常颖 1,1; 王狮凌 2
作者单位
摘要
1 长春理工大学光电工程学院, 吉林 长春 130022
2 天津大学精密测试技术及仪器国家重点实验室, 天津 300072
设计了一块球面-非球面柱透镜,用于将高斯圆斑整形为平顶线斑。通过编写Zemax编程语言批量添加操作数与设置默认优化函数优化结合的方法完成设计,并与性能参数相同的非球面透镜-柱透镜组进行比较,同时分析了球面-非球面柱透镜最后一面到像面距离的不同对线斑长宽比和平顶度的影响。与非球面透镜-柱透镜组相比,线斑尺寸相同但平顶度一般(边缘处约下降10%),在一定范围内调整最后一面到像面的距离可使平顶度变好(可达到90%),但会使长宽比变小(由88.33降至20.38)。所得结果表明,若要获得能量均匀分布的线斑,在长宽比可调整的范围内,球面-非球面柱透镜的设计可以简化光束整形系统结构,满足轻量化的要求,是一种可行的方法。
几何光学 激光光束整形 非球面透镜设计 非成像光学系统 
激光与光电子学进展
2018, 55(6): 060801
作者单位
摘要
南京信息工程大学气象灾害预警与评估协同创新中心,中国气象局气溶胶-云-降水重点实验室,教育部气象灾害重点实验室,南京 210044
为进一步了解云物理过程,探测冰云及混合相云云粒子特性,提出了一种带有偏振通道的云粒子探测器模型,可以同时探测前向散射和后向散射一定立体角内的散射能量和退偏比。模拟了椭球,圆柱和球形粒子的相函数,不同角度的退偏比,总散射截面,发现球形粒子几乎不产生退偏,其退偏与椭球、圆柱粒子退偏有数个量级的差距,探测时可以直接以退偏分辨球形粒子。计算了在探测器前后两个接收立体角内非球形粒子的散射截面和退偏比均值,粒子退偏比和散射截面随粒子的横纵比变化比较连续,一定条件下可以分辨部分粒子的形状。粒子退偏比随粒子的等效半径变化波动,不利于探测时分辨粒子大小。在模拟的粒径范围内,粒子等效半径和散射截面大致成正相关,探测时可以以此分辨粒子大小。粒子散射模拟结果表明,该探测系统除可以进行球形粒子探测能力外,具有一定的非球形粒子探测能力。
T矩阵 云粒子探测 偏振激光探测 非球形粒子 光散射 T-Matrix cloud detection polarized laser nonspherical particle light scattering 
光散射学报
2018, 30(2): 174
胡帅 1高太长 1,2,*刘磊 1李浩 1[ ... ]洪昌伟 3
作者单位
摘要
1 国防科技大学气象海洋学院, 江苏 南京 211101
2 解放军陆军工程大学电磁环境效应与光电工程国家级重点实验室, 江苏 南京 210007
3 解放军95019部队, 湖北 老河口 441800
非球形气溶胶穆勒散射矩阵的不确定性是影响偏振遥感精度的重要因素。在自主研制的时域多分辨率(MRTD)气溶胶散射模型中,穆勒散射矩阵的计算需要以远场电场值为基础,因此近远场外推过程成为制约其模拟精度的重要环节。为确定适用于MRTD散射模型的最佳近远场外推方案,在球形和非球形粒子情形下,系统地对比分析了基于惠更斯原理的表面积分方案以及基于电介质亥姆霍兹方程的体积积分方案所对应的穆勒散射矩阵的模拟精度。结果表明,虽然两种近远场外推方案均可有效准确地实现近远场外推,但从穆勒矩阵的计算误差分布上看,基于体积积分原理的近远场外推方案性能更优。
散射 非球形气溶胶 近远场外推 穆勒散射矩阵 散射模型 
光学学报
2018, 38(6): 0629002
Author Affiliations
Abstract
State Key Laboratory of Precision Measurement Technology and Instruments, Department of Precision Instrument, Tsinghua University, Beijing 100084, China
In this Letter, we present a novel design method of image-side telecentric freeform imaging systems. The freeform surfaces in the system can be generated using a point-by-point design approach starting from an initial system consisting of simple planes. The proposed method considers both the desired object–image relationships and the telecentricity at the image-side during the design process. The system generated by this method can be taken as a good starting point for further optimization. To demonstrate the benefit and feasibility of our method, we design two freeform off-axis three-mirror image-side telecentric imaging systems in the visible band. The systems operate at F/1.9 with a 30 mm entrance pupil diameter and 5° diagonal field-of-view. The modulation-transfer-function curves are above 0.69 at 100 lps/mm.
220.2740 Geometric optical design 080.4225 Nonspherical lens design 
Chinese Optics Letters
2017, 15(6): 062202
王玉文 1,*董志伟 1,2,3
作者单位
摘要
1 中国工程物理研究院研究生院北京 100088, 四川 绵阳 621999
2 中国工程物理研究院 微系统与太赫兹研究中心, 四川 绵阳 621999
3 北京应用物理与计算数学研究所, 北京 100094
水汽凝结体对太赫兹波在大气中的传输衰减起重要作用。结合 T-matrix方法, 数值模拟了云层中非球形冰晶在太赫兹波段的吸收和散射效应, 建立了对称性非球形冰晶的太赫兹波衰减统计模型。分析了不同结构的非球形冰晶的消光特性, 对比 MPM模型的球形水云衰减, 结果显示太赫兹波段对称非球形冰晶的散射特性明显, 衰减效应强于球形水滴, 衰减系数平均为 20 dB左右, 1 THz以上消光截面随冰晶形状的变化而变化, 为太赫兹星地通信提供了参考数据。
太赫兹波 对称非球形冰晶 衰减 T-matrix方法 Terahertz wave nonspherical symmetric ice crystal attenuation T-matrix 
太赫兹科学与电子信息学报
2017, 15(3): 345
胡帅 1高太长 1,2李浩 1杨波 2[ ... ]李刚 3
作者单位
摘要
1 解放军理工大学气象海洋学院, 江苏 南京 211101
2 解放军理工大学电磁环境效应与光电工程国家级重点实验室, 江苏 南京 210007
3 中国洛阳电子装备实验中心, 河南 洛阳 471000
为解决串行时域多分辨率(MRTD)散射模型运行时间长和内存消耗大的问题, 基于消息传递接口(MPI)技术设计了一种非球形气溶胶散射并行计算模型。介绍了MRTD散射模型的基本框架和2种并行数据通信方案, 并基于MPI重复非阻塞通信技术实现了MRTD散射模型的并行化设计; 搭建了网络并行计算平台, 实现了模型的并行化计算。将MRTD散射模型与Mie散射模型、T矩阵法进行了对比, 验证了并行MRTD散射模型的计算准确性。结果表明, MRTD模型可较准确地模拟非球形粒子散射特性, 并行计算技术可显著提高计算效率; 电磁场分量同时交换的并行设计方案的计算效率略高于仅交换磁场分量的方案; 通过增加中央处理器核数, 程序的并行加速比随之增大, 但单核运行效率却略有降低。随着粒子尺度参数的增大, 单核计算效率随之增加, 复折射率的改变并不会显著影响并行计算效率。
大气光学 非球形气溶胶 散射 时域多分辨率 并行计算 
光学学报
2017, 37(6): 0601001
Author Affiliations
Abstract
State Key Laboratory of Precision Measurement Technology and Instruments, Department of Precision Instrument, Tsinghua University, Beijing 100084, China
In this Letter, a novel and compact freeform off-axis three-mirror imaging system and its detailed design method are proposed. The primary mirror and tertiary mirror of the system have the same surface analytical expression and they are integrated on one single freeform surface. In this way, the alignment process is made much easier due to the much fewer degrees of freedom. In addition, the difficulty and cost for the data handling, fabrication, and testing of the freeform surfaces and system can also be significantly reduced in some cases, especially compared with the configuration having multiple surfaces of different expressions integrated on one monolithic substrate. The final system has a 100 mm effective focal length and a 4°×3° field of view. The modulation transfer function of the system is close to the diffraction-limit.
220.2740 Geometric optical design 080.4225 Nonspherical lens design 080.4228 Nonspherical mirror surfaces 
Chinese Optics Letters
2016, 14(6): 060801
Author Affiliations
Abstract
State Key Laboratory of Precision Measurement Technology and Instruments, Department of Precision Instrument, Tsinghua University, Beijing 100084, China
In this Letter, we propose a novel configuration and design method of freeform, dual fields-of-view (FOVs), dual focal lengths, off-axis three-mirror zoom imaging systems. The switch of the two zooms is achieved by rotating a single mirror element. The design of a freeform, dual focal lengths zoom system is realized by a point-by-point design approach for the first time to our knowledge. This method enables the direct design of freeform surfaces from initial planes using given system specifications and configuration, and the designed system can be taken as a good starting point for further optimization. A freeform, dual FOVs, dual focal lengths, off-axis three-mirror zoom system is demonstrated. The F-numbers of the two zooms are 2 and 2.4. The dual FOVs are 3°×3° and 2.5°×2.5°. After final optimization, both of the zooms achieve high performances.
080.4228 Nonspherical mirror surfaces 080.4035 Mirror system design 220.2740 Geometric optical design 
Chinese Optics Letters
2016, 14(10): 100801

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