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。
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
Uni Optics平凹圆柱面镜在垂直方向上具有凹面曲率，在水平方向上无曲率。它们边缘呈圆形，因此在光学系统中很容易与其他元件结合。
1. 为什么使用柱面镜？
柱面镜通常用于聚焦、凝聚或扩展入射光。柱面镜有一个柱面，使光聚焦在一个尺寸或轴上。
2. 使用圆柱面镜可以纠正眼睛哪些缺陷？
用柱面镜可以矫正眼睛的散光缺陷。散光是由于晶状体曲率不均匀造成。
产品规格
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：≤3弧分
表面质量：40-20 s/d
表面平整度：n=5△n=0.5
通光孔径：>90%
镀膜：可选泽性（无镀膜/单层MGF2镀膜/宽带AR镀膜）
| Part NO. | Material | F(mm) | Φ(mm) | R(mm) | Tc(mm) | Te(mm) | Fb(mm) |
|---|---|---|---|---|---|---|---|
| ULYRPV008005 | BK7 | -8 | 5 | -4.13 | 2 | 2.84 | -9.34 |
| ULYRPV092008 | BK7 | -9.2 | 8 | -4.74 | 2 | 4.2 | -10.53 |
| ULYRPV010008 | BK7 | -10 | 8 | -5.16 | 2 | 3.89 | -11.31 |
| ULYRPV125127 | BK7 | -12.5 | 12.7 | -6.43 | 2 | 7.44 | -13.8 |
| ULYRPV025127 | BK7 | -25 | 12.7 | -12.89 | 2 | 3.67 | -26.33 |
| ULYRPV050127 | BK7 | -50 | 12.7 | -25.76 | 2 | 2.8 | -51.33 |
| ULYRPV075254 | BK7 | -75 | 25.4 | -38.64 | 2 | 4.15 | -76.34 |
| ULYRPV100254 | BK7 | -100 | 25.4 | -51.52 | 3 | 4.59 | -102 |
| ULYRPV150254 | BK7 | -150 | 25.4 | -77.27 | 3 | 4.05 | -151.99 |
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平凹方形柱面镜
高功率激光窗片
1.什么是激光窗片
激光防护窗，也称为激光防护玻璃、防护滤光片或焊接防护窗，主要应用于保护高成本的激光光学元件，以节省资金。
2.激光窗的主要用途是什么？
这些窗口片通常用于激光切割、激光焊接等设备上，用以避免高精度的激光光学器件因加工时材料飞溅而造成的损坏。
3.优恩立激光窗口片的主要优势
高传输率
高损伤阈值
低散射
低吸收
优良的膜层密度
良好的环境稳定性
常规规格：
尺寸：4-80毫米，圆形或方形
材质：BK7、熔融石英、ZnSe等
表面质量：10/5
面型：lambda/10@632.8nm
平行度：30''
粗糙度：3A
N-BK7五角棱镜
在光学系统中，五棱镜是用来定义直角的，它能够提供右手图像，特点是使光线偏离90°。五角棱镜是具有五个面的棱镜，不受轻微运动的影响。福州优恩立光电提供多种五角棱镜，在紫外，可见光，和红外光谱范围具有良好的光学性能。
可视光/近红外镀膜的双凹透镜
双凹透镜是一种带有两个凹面的负焦距的光学透镜，常用于光束扩展、图像缩小或光投影等应用，也是扩大光学系统焦距的理想选择。优恩立公司可为您提供广泛用途的，带有多种涂层的双凹透镜。
融石英球透镜和半球透镜
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.
电话 : +86-591-86395085
电子邮件 : sales@uni-optics.com
