产品
Home /

柱面镜

/光学玻璃平凸圆柱形透镜

光学玻璃平凸圆柱形透镜

平凸圆形柱面镜可用于各种应用中的线性成像或单轴放大。可以与其他镜头组合以形成复杂的成像系统。

  • 产品产地:

    中国
  • 航运港口:

    中国福州
  • 交付周期:

    四周
  • 付款:

    银行电汇, 西联付款
立即查询
  • 描述


 Uni Optics的平凸圆形柱面镜在垂直方向上具有凸曲率,在水平方向上没有曲率。它们被修边为圆形,因此可以很容易地与光学系统中的其他原件组合应用。


 


1. 如何正确控制半径曲率?


Uni Optics使用精密模板进行加工处理,以确保最终的R值与您的图纸相匹配。




2. 能提供测试报告吗?



可以。我们可以提供实测数据,包括半径曲率,中心,尺寸,表面质量,镀膜曲线等。



 

 Plano-Convex Circular Cylindrical Lenses  Plano-Convex Circular Cylindrical Lenses



通用规格

材料:Schott,CDGM,Ohya,Ohara,Corning等

直径公差:+ 0 / -0.05mm

有效焦距公差:±2%

中心偏公差:≤3弧分

表面质量:40-20 S / D.

表面面型:N = 5△N = 0.5

通光孔径:> 90%的表面尺寸

涂层:可选(无涂层/单层MgF2 /AR等)




Part NO. Material F(mm) Φ(mm) R(mm) Tc(mm) Te(mm) Fb(mm)
ULYRPX008005 BK7 8 5 4.13 2.84 2 6.14
ULYRPX092008 BK7 9.2 8 4.74 4.2 2 6.44
ULYRPX010008 BK7 10 8 5.17 3.9 2 7.43
ULYRPX125127 BK7 12.5 12.7 6.43 7.44 2 7.57
ULYRPX025127 BK 25 12.7 12.88 3.67 2 22.58
ULYRPX050127 BK7 50 12.7 25.75 2.8 2 48.17
ULYRPX075254 BK7 75 25.4 38.64 4.15 2 72.28
ULYRPX100254 BK7 100 25.4 51.52 4.59 2 96.99
ULYRPX150254 BK7 150 25.4 77.27 4.05 2 147.34


发送消息
如果您在使用本网站或我们的产品时有任何问题,请写下您的意见或建议,我们将尽快回答您的问题!感谢您的关注!
如果您有任何问题或建议,请给我们留言,我们会尽快回复您!
相关产品
BK7平凸方形柱面镜
平凸方形柱面镜
平凸矩形柱面透镜可用于广泛应用中的线性成像或单轴放大。 这些镜头可以与其他镜头组合以形成复杂的成像系统。
平凹方形柱面镜供应商
平凹方形柱面镜

平凹矩形柱面镜为合成光束扩散及其广泛应用提供了单轴负成像。如果需柱面镜凹面作为反射镜,这些透镜可用作镜坯。



定制平凹圆型柱面镜
平凹圆型柱面镜

平凹柱面镜为合成光束扩散及其广泛应用提供了单轴负成像。如果需要柱面镜凹面作为反射镜,这些透镜可用作镜坯。

BK7镀增透膜窗片
BK7镀增透膜窗片

BK7窗口是最常见的窗口类型。在可见光和近红外波段具有良好的性能。同时,BK7窗口是理想的应用需要最小的传输光束偏差。适用于AR涂层。

鍺窗口片
红外窗口片鍺窗口片
锗是8-12微米波段高性能红外成像系统的首选镜头和窗口材料。其高折射率使Ge成为低功率成像系统的理想选择。色差很小,通常不需要校正。
镀增透膜有色玻璃滤光片
高精度有色玻璃滤光片

有色玻璃滤光片是通过吸收在玻璃中分布的光学物质来控制入射波长的光学原件。

微型元件棒透镜
棒透镜

用于光纤耦合和激光二极管光束成形,工作距离为0mm的透镜非常适用于单模和多模光纤和激光二极管的准直,因为透镜可以直接定位并直接粘合在发射源上。 对于聚焦应用,或者镜头不能与发射源直接接触的情况下,所有镜头也可以具有小的工作距离。UNI Optics可提供Φ1~Φ15mm的尺寸,数量和尺寸,包括抛光/磨削表面的差异,可根据客户要求提供。

Laser Crystal
激光晶体

晶体最适用于激光应用。 UNI OPTICS提供以下晶体产品。

1.激光晶体和棒:YAG晶体,Nd:YVO4晶体
2.非线性晶体:BBO,KTP,LiNbO3,LBO。KDP&DKDP
3.双折射晶体:YVO4,a-BBO,方解石。


IR Optics material
红外材料

1.  Germanium (Ge)


Germanium (Ge) is the preferred lens and window material for high performance infrared imaging systems in the 8–12 μm wavelength band. Its high refractive index makes Ge ideal for low power imaging systems because of minimum surface curvature. Chromatic aberration is small, often eliminating the need for correction.

 

Crystallographic properties
Syngony Cubic
Crystal Form Poly or Single Crystal
Lattice Constant 5.66
Cleavability <111>, non-perfect
Molecular Weight 72.6
Physical properties
Density, at 20 °C 5.33
Hardness, Mohs 6.3
Dielectric Constant for 9.37 × 109 Hz at 300 K 16.6
Melting 937
Thermal Conductivity, W/m·K at at 293 K 59
Thermal Expansion, 1/K at 298 K 6.1 × 10-6
Specific Heat Capacity, J/(kgK) at 273-373 K 0.074
Bandgap, eV 0.67
Knoop Hardness, kg/mm2 800
Youngs Modulus, Gpa 102.66
Shear Modulus, GPa 67.04
Bulk Modulus, GPa 77.86
Debye Temperature, K 370
Poissons Ratio 0.278
Elastic Coefficient C11=129, C12=48.3, C44=67.1
Apparent Elastic Limit 89.6 MPa (13000psi)
Chemical properties
Solubility in water None
Solubility in acids Soluble
Molecular Weight 72.59

2. Silicon (Si) 


Silicon (Si) is grown by Czochralski pulling techniques (CZ) and contains some oxygen that causes an absorption band at 9 microns.To avoid this, material can be prepared by a Float-Zone (FZ) process. Optical silicon is generally lightly doped (5 to 40 ohm cm) for best transmission above 10 microns, and doping is usually boron (P-type) and phosphorus (N-type). After doping silicon has a further pass band: 30 to 100 microns which is effective only in very high resistivity uncompensated material.
 
CZ Silicon is commonly used as substrate material for infrared reflectors and windows in the 1.5-8 micron region. The strong absorption band at 9 microns makes it unsuitable for CO2 laser transmission applications, but it is frequently used for laser mirrors because of its high thermal conductivity and low density. Application as window, lens in the 1.5 - 8 um region; Mirror for CO2 laser and spectrometer applications.
 

Crystallographic properties
Syngony Cubic
Lattice Constant, A 5.43
Physical properties
Density 2.33g/cm3
Hardness, Mohs 7
Dielectric Constant for 9.37 x 109 Hz 13
Melting point, оС 1414
Thermal Conductivity, W/m·K at 313 K 163
Thermal Expansion, 1/K at 293 K 2.6x10-6
Specific Heat Capacity, J/(kg°C) 712.8
Bandgap, eV 1.1
Knoop Hardness, kg/mm2 1100
Youngs Modulus, Gpa 130.91
Shear Modulus, GPan 79.92
Bulk Modulus, GPa 101.97
Debye Temperature, K 640
Poissons Ratio 0.28
Chemical properties
Solubility in water None
Molecular Weight 28.09

3、ZnS material:


ZnS MultiSpectral Under intense heat and pressure, defects within the crystalline lattice are virtually eliminated, leaving a water-clear material with minimal scatter and high transmission characteristics from 0.4 to 12 microns. This material is particularly well suited for high-performance common aperture systems that must perform across a broad wavelength spectrum.

Specifications:

Material: ZnS MultiSpectral
Diameter Tolerance: --------------------- +0.0, -0.1mm
Thickness Tolerance: -------------------- ±0.1mm
Clear Aperture: ---------------------------->85%
Parallelism: -----------------------------------3 arc minute
Surface Quality: ----------------------------80-50 scratch and dig
Wavefront Distortion: -------------------- λ /2 per 25mm @633mm
Bevel: -----------------------------------------Protective  (<0.2mm x 45° )
Coating: -------------------------------------- Optional (Uncoated, AR Coating, etc.)


4. ZnSe material


ZnSe is a preferred material for lenses, windows, output couplers and beam expanders for its low absorptivity at infrared wavelengths and its visible transmission. For high-power applications, it’s critical that the material bulk absorption and internal defect structure be carefully controlled, that minimum-damage polishing technology be employed, and the highest quality optical thin-film coatings are used. The material absorption is verified by CO2 laser vacuum calorimetry. Our quality assurance department provides testing and specific optics certification on request.

ZnSe is non-hygroscopic and chemically stable, unless treated with strong acids. It’s safe to use in most industrial field, and laboratory environments.



融石英楔角棱镜
N-BK7和融石英楔角棱镜

棱镜是一种具有平面倾斜面的光学元件,通常各面以很小的角度相互倾斜,它将光线转向较厚的部分通常可以用作隔离元件。楔角棱镜也可以用来产生一个小偏差,不允许光线返回源。

装配的带通滤光片
机器视觉带通滤光片


带通滤光片是一种通过一定范围内的频率并拒绝(衰减)该范围之外频率的装置,它用于选择性地传输一部分光谱,同时拒绝所有其他波长


UN Grade Fused Silica
融石英
融石英由硅和氧的化学结合形成。 熔融石英是一种完美的光学材料,因为它具有良好的紫外和红外透射率,低热膨胀系数。 它具有高稳定性,耐大温度偏移,宽温度工作范围和高激光损伤阈值的热冲击。
订阅我们的通讯
联系
请求免费报价
如果您在使用本网站或我们的产品时有任何问题,请写下您的意见或建议,我们将尽快回答您的问题!感谢您的关注!

版权 © 福州优恩立光电科技有限公司 © 保留所有权利.

留言

首页

产品

公司

联系