欧美成人午夜激情视频_亚洲视频第一页_日韩免费看的电影电视剧大全_欧美黄色片视频_欧美性色视频在线_亚洲第一福利视频_欧美亚洲激情视频_成人欧美在线视频_亚洲综合一区二区不卡_国产91精品久久久久久久_成人午夜两性视频_日韩欧美在线视频免费观看_久久人人爽人人_国产成人综合久久_国产精品久久久久9999_久久99热精品这里久久精品

撥號18861759551

你的位置:首頁 > 技術文章 > 使用塑料混合非球面透鏡的優點

技術文章

使用塑料混合非球面透鏡的優點

技術文章

Advantages of Using Plastic Hybrid Aspheric Lenses

TECHSPEC® Plastic Hybrid Aspheric Lenses are low cost optical components that lack both spherical and chromatic aberrations. These aspheric lenses provide optical designers with unique, single element solutions for achieving diffraction-limited focusing performance at high numerical apertures with broadband light sources. These aspheric lenses consist of a diffractive surface that has been added to a molded aspheric lens. The aspheric lens eliminates all spherical aberration, while the diffractive surface has a net effect of introducing negative dispersion – when properly tuned to the refractive index and wavelength design of the lens, chromatic aberration is eliminated as well.

 

Spherical and Chromatic Aberrations

There are two major forms of axial optical aberrations inherent in common optical lenses: spherical aberration and chromatic aberration. Spherical aberration is an inherent characteristic of any lens whose surface is a section of a sphere. Light originating from the same object point comes to a focus at slightly different points (P and P’), depending on whether the rays pass through the center of the lens or the periphery (Figure 1).

Figure 1: Spherical Aberration in a Single Positive Lens

 

igure 2.1: Transverse Chromatic Aberration of a Single Positive Lens

 

Figure 2.2: Longitudinal Chromatic Aberration of a Single Positive Lens

 

Chromatic aberration results from material dispersion. Because different colors of light refract by different amounts, an image point formed by light of one color does not coincide with the corresponding image point formed by light of a different color (Figures 2.1 and 2.2).

 

Important Equations

Spherical aberration is typically eliminated by substituting an aspherical surface for the more common spherical surface. The surface profile (sag) is given by Equation 1:

Where

Z = sag of surface parallel to the optical axis

s = radial distance from the optical axis

C = curvature, inverse of radius

k = conic constant

A4, A6, A8 = 4th, 6th, 8th… order aspheric terms

 

However, this does not correct chromatic aberration. Therefore, for a monochromatic light source, the aspheric surface will provide diffraction limited focusing at a single wavelength, but will suffer a large spot size over a broader wavelength.

 

A diffractive surface will correct the spherical aberration, as shown in Equation 2.

Where
Y = radial position from center of lens (for instance, if 0 is the center of the lens, 12.5mm will be the edge of a 25mm diameter lens, etc.)
nd = index of refraction of the material at 587.6nm
Step Height = λ/nd-1
λ = the wavelength of interest

By combining the two features onto a single element, a component that eliminates both chromatic and spherical aberration is created. That surface is described simply as the sum of the Zasph and Zdiff coefficients.

For tips on modeling diffractives in Zemax and Code V, visit the Optics Realm blog.

 

Customer Benefits

Optical designers often need to focus light at very short distances, or collect and collimate as much light as possible from very divergent light sources. Basic optical principles dictate that a high numerical aperture optical lens is required for either of these scenarios. A high numerical aperture optical lens will typically have a focal length equal to or shorter than the clear aperture of the optical system, allowing the designer to maintain as compact of an optical train as possible.

For example, an optical designer has multiple options for achieving a focal length that is equal to his clear aperture (a scenario known as an F/1 lens, or a lens with a numerical aperture of 0.50). The simplest option is to use a standard plano-convex lens, available from a number of distributors. Spot diagram, chromatic focal shift graph, polychromatic diffraction MTF, and transverse ray fan plot for the wavelength range of 486 - 656nm are provided for #45-097 25mm Diameter x 25mm FL PCX lens.

 

PCX Lens

Figure 3.1: Spot Diagram for #45-097 25mm Dia. x 25mm FL PCX Lens

Figure 3.2: Chromatic Focal Shift Graph for #45-097 25mm Dia. x 25mm FL PCX Lens

Figure 3.3: Polychromatic Diffraction MTF Graph for #45-097 25mm Dia. x 25mm FL PCX Lens

Figure 3.4: Transverse Ray Fan Plot for #45-097 25mm Dia. x 25mm FL PCX Lens

 

For improved performance, the optical designer could consider an achromatic lens of the same form factor, for example #65-553 25mm Diameter x 25mm Focal Length Achromatic Lens. Again, the same characteristics are shown over the same wavelength range. A 74% decrease in spot size with a 73% decrease in chromatic focal shift can be seen, yielding an MTF of 13 lp/mm at 40% contrast, a substantial gain versus the aforementioned singlet lens.

Figure 4.1: pot Diagram for #65-553 25mm Dia. x 25mm FL Achromatic Lens

Figure 4.2: Chromatic Focal Shift Graph for #65-553 25mm Dia. x 25mm FL Achromatic Lens

Figure 4.3: Polychromatic Diffraction MTF Graph for #65-553 25mm Dia. x 25mm FL Achromatic Lens

Figure 4.4: Transverse Ray Fan Plot for #65-553 25mm Dia. x 25mm FL Achromatic Lens

For maximum performance, the optical designer should choose a plastic hybrid aspheric lens. In this scenario, the exact same form factor and wavelength range are used, this time with #65-992 25mm Diameter x 25mm FL Hybrid Aspheric Lens. As shown, this lens provides diffraction limited focusing performance, yielding the optimum performance for the designer.

 

Plastic Hybrid Lens

Figure 5.1: Spot Diagram for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

Figure 5.2: Chromatic Focal Shift Graph for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

Figure 5.3: Polychromatic Diffraction MTF Graph for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

Figure 5.4: Transverse Ray Fan Plot for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

Comparing the spot diagrams, chromatic focal shift graphs, polychromatic diffraction MTFs, and transverse ray fan plots of a plano-convex (PCX) lens, achromatic lens, and hybrid aspheric lens, it is easy to see the advantages of using plastic hybrid aspheric lenses for achieving diffraction-limited focusing performance at high numerical apertures with broadband light sources.

 

Selection Guide

Edmund Optics® TECHSPEC® Plastic Aspheres and TECHSPEC® Plastic Hybrid Aspheres families are both manufactured utilizing Zeon Chemical’s Zeonex E48R material. Zeonex materials feature high transparency, low fluorescence, low birefrengence, low water absorption, and high heat and chemical resistance, making it a superior material vs. other commonly available plastics. Zeonex is a Cylco Olefin Polymer (COP) material.

Plastic Materials Selection Guide

Property

Glass

Zeonex E48R

PMMA

Polycarbonate

Polystyrene

Arton®

Transmission

Excellent

Excellent

Excellent

Good

Very Good

Excellent

Low Refractive Index

Excellent

Excellent

Excellent

Poor

Poor

Good

Low Birefringence

Excellent

Excellent

Excellent

Poor

Poor

Excellent

Low Water Absorption

Excellent

Excellent

Poor

Good

Excellent

Excellent

Impact Resistance

Poor

Good

Good

Excellent

Good

Excellent

Moldability

Fair

Excellent

Good

Excellent

Excellent

Good

Heat Resistance

Excellent

Good

Poor

Good

Poor

Very Good

Coating Adhesion

Excellent

Good

Fair

Fair

Fair

Good

聯系我們

地址:江蘇省江陰市人民東路1091號1017室 傳真:0510-68836817 Email:sales@rympo.com
24小時在線客服,為您服務!

版權所有 © 2025 江陰韻翔光電技術有限公司 備案號:蘇ICP備16003332號-1 技術支持:化工儀器網 管理登陸 GoogleSitemap

在線咨詢
QQ客服
QQ:17041053
電話咨詢
0510-68836815
關注微信
欧美成人午夜激情视频_亚洲视频第一页_日韩免费看的电影电视剧大全_欧美黄色片视频_欧美性色视频在线_亚洲第一福利视频_欧美亚洲激情视频_成人欧美在线视频_亚洲综合一区二区不卡_国产91精品久久久久久久_成人午夜两性视频_日韩欧美在线视频免费观看_久久人人爽人人_国产成人综合久久_国产精品久久久久9999_久久99热精品这里久久精品
欧美国产精品va在线观看| 91情侣偷在线精品国产| 国产成人自拍视频在线观看| 亚洲精品动漫久久久久| 成人午夜在线影院| 欧美视频裸体精品| 欧美视频在线免费看| 久久香蕉国产线看观看av| 欧美亚洲日本网站| 日韩精品免费看| 欧美一区二三区| 夜夜嗨av色综合久久久综合网| 久久久久久久久久久成人| 中文字幕亚洲欧美在线| 亚洲精品资源美女情侣酒店| 久久人人爽人人| 日韩中文字幕在线观看| 一区二区福利视频| 日韩最新av在线| 精品人伦一区二区三区蜜桃免费| 精品性高朝久久久久久久| 国产精品久久久久久久久影视| 久久露脸国产精品| 久久久久久久久久国产| 国产一区二区三区在线播放免费观看| 6080yy精品一区二区三区| 国产成人aa精品一区在线播放| 成年无码av片在线| 亚洲午夜小视频| 久久久国产一区| 欧美激情videoshd| 亚洲已满18点击进入在线看片| 欧美精品免费播放| 亚洲wwwav| 国产日韩在线看片| 疯狂做受xxxx高潮欧美日本| 欧美激情免费视频| 成人免费视频在线观看超级碰| 日韩经典中文字幕在线观看| 亚洲美女又黄又爽在线观看| 欧美日韩午夜激情| 久久琪琪电影院| 国产精品一区二区性色av| 日韩美女免费视频| 91国自产精品中文字幕亚洲| 亚洲一区二区少妇| 久久99国产精品久久久久久久久| 久久人人97超碰精品888| 国产视频在线一区二区| 久久夜色精品国产| 日本sm极度另类视频| 岛国av一区二区三区| 日韩小视频网址| 欧美性一区二区三区| 亚洲精品电影久久久| 亚洲一区二区三区在线视频| 久久人人爽人人爽人人片av高请| 亚洲天堂av女优| 日韩在线精品一区| 波霸ol色综合久久| 亚洲欧美国产一区二区三区| 色偷偷888欧美精品久久久| 欧美高跟鞋交xxxxhd| 国产在线观看精品| 精品女厕一区二区三区| 欧美日韩国产一区中文午夜| 欧美激情视频一区二区三区不卡| 日韩成人在线视频网站| 日韩中文在线不卡| 久久精品电影网| 55夜色66夜色国产精品视频| 黄色一区二区在线观看| 精品国产美女在线| 亚洲免费福利视频| 欧美日韩美女视频| 亚洲精品中文字幕av| 亚洲激情 国产| 亚洲欧美制服综合另类| 久久久久久这里只有精品| 国产一区二区在线免费| 日韩精品久久久久久福利| 国产精品影院在线观看| 亚洲第一综合天堂另类专| 国产91色在线播放| 亚洲精品乱码久久久久久按摩观| 久久福利视频网| 色综合老司机第九色激情| 久久综合亚洲社区| 秋霞成人午夜鲁丝一区二区三区| 国外成人免费在线播放| 情事1991在线| 亚洲综合视频1区| 黑人欧美xxxx| 国产精品高潮呻吟久久av无限| 成人乱色短篇合集| 国产精品久久久久av免费| 亚洲午夜激情免费视频| 搡老女人一区二区三区视频tv| 亚洲成人av中文字幕| 国产亚洲欧美日韩一区二区| 精品视频在线播放免| 亚洲欧美国产精品久久久久久久| 久久亚洲一区二区三区四区五区高| 久久99热这里只有精品国产| 国产欧美一区二区三区久久人妖| 三级精品视频久久久久| 久久精品99久久久久久久久| 欧美放荡办公室videos4k| 国产欧美欧洲在线观看| 欲色天天网综合久久| 国产精品久久久久秋霞鲁丝| 精品国产电影一区| 久久激情五月丁香伊人| 亚洲欧美制服丝袜| 亚洲视频一区二区三区| 久久久视频精品| 这里只有精品久久| 日韩在线观看免费网站| 在线日韩精品视频| 日韩成人久久久| 亚洲欧美日本精品| 亚洲人成在线播放| 国产精品九九久久久久久久| 亚洲欧美一区二区三区久久| 91夜夜揉人人捏人人添红杏| 欧美日韩激情视频8区| 久久亚洲精品视频| 午夜精品一区二区三区在线视| 久久影院在线观看| 欧美视频在线观看免费网址| 亚洲精品久久久久中文字幕欢迎你| 亚洲精品ady| 黄色成人av在线| www.日韩av.com| 日韩免费av一区二区| 国产99在线|中文| 久久视频这里只有精品| 国产精品一区二区久久久| 色www亚洲国产张柏芝| 国产精品久久9| 久久理论片午夜琪琪电影网| 九九热视频这里只有精品| 精品久久久久久国产91| 午夜精品久久久久久久白皮肤| 久久国产精品99国产精| 精品久久久久久久久久国产| 欧美激情va永久在线播放| 欧美成人免费一级人片100| 欧美亚洲成人xxx| 欧美精品videosex极品1| 亚洲综合在线小说| 日韩免费av一区二区| 国产97人人超碰caoprom| 中文字幕精品一区久久久久| 久久久国产精品视频| 日韩中文字幕免费视频| 色综合视频一区中文字幕| 久久精品国产v日韩v亚洲| 亚洲色图在线观看| 精品福利在线看| 日韩在线免费av| 精品久久久香蕉免费精品视频| 亚洲国产精品久久久久秋霞蜜臀| 久久人人爽人人爽人人片av高请|