<label id="kuzok"></label>

  • 
    
    <span id="kuzok"><noframes id="kuzok"><label id="kuzok"></label>
  • <li id="kuzok"><tbody id="kuzok"><th id="kuzok"></th></tbody></li>
    <label id="kuzok"></label>
    <rt id="kuzok"></rt>
    <bdo id="kuzok"><meter id="kuzok"></meter></bdo>

    <center id="kuzok"><optgroup id="kuzok"></optgroup></center>
    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
    主站蜘蛛池模板: 国产综合在线观看| 亚洲国产精品成人综合色在线婷婷| 亚洲综合激情另类小说区| 亚洲综合久久一本伊伊区| 色综合久久98天天综合| 亚洲综合网站色欲色欲| 天天躁日日躁狠狠躁综合| 亚洲另类激情综合偷自拍图| 欧美日韩综合一区二区三区| 狠狠色婷婷狠狠狠亚洲综合| 亚洲妓女综合网99| 综合国产精品第一页| 一本久道综合色婷婷五月| 国产成人亚洲综合色影视| 亚洲综合另类小说色区色噜噜| 天天影视色香欲综合免费| 亚洲丁香色婷婷综合欲色啪| 国产成人亚洲综合| 日日狠狠久久偷偷色综合0| 色狠狠成人综合色| 色妞色综合久久夜夜| 亚洲国产综合无码一区| 亚洲国产精品成人AV无码久久综合影院| 亚洲综合色7777情网站777| 亚洲五月激情综合图片区| 久久一日本道色综合久久m| 激情97综合亚洲色婷婷五| 综合亚洲伊人午夜网| 亚洲情综合五月天| 亚洲综合婷婷久久| 亚洲国产精品综合久久20| 97se色综合一区二区二区| 丁香婷婷激情综合俺也去| 色综合久久久无码中文字幕波多| 狠狠色丁香久久婷婷综合图片| 亚洲综合在线成人一区| 色综合久久久无码中文字幕波多| 国产成人综合久久精品| 狠狠色狠狠色综合| 亚洲国产欧美国产综合一区| 一本久道久久综合多人|