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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。
  • 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
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  • 描述

为什么使用平凸柱面镜?

平凸矩形柱面透镜可提供正焦距或负焦距,非常适用于激光线生成或变形光束整形,可在各种应用中单轴放大,使激光输出圆形化。这些透镜可与其他透镜组合形成复合体 成像系统。



Plano-convex rectangular Cylindrical Lenses  Plano-convex rectangular Cylindrical Lenses


参数: 


材料: 光学玻璃,融石英
设计波长: 546.1nm
直径公差: +0/-0.05mm
焦距公差: +/-2%
光洁度: 40-20 S/D
中心偏: 3 arcmin
面形: N=5 △N=0.5
通光孔径: 90%
倒边: Protective
镀膜 Optional



Part NO. Material W x H F(mm) R(mm) Tc(mm) Te(mm) Fb(mm)
ULYPX1010127 BK7 10.0x10.0 12.7 6.54 4.3 2 9.8
ULYPX1010020 BK7 10.0x10.0 20.0 10.29 3.3 2 17.8
ULYPX1010025 BK7 10.0x10.0 25.0 12.87 3.0 2 23
ULYPX1210010 BK7 12.0x10.0 10.0 5.2 5.9 2 6.17
ULYPX1210015 BK7 12.0x10.0 15.0 7.8 3.8 2 12.6
ULYPX1210020 BK7 12.0x10.0 20.0 10.34 3.3 2 17.8
ULYPX2010127 BK7 20.0x10.0 12.7 6.54 , 4.3 2 9.8
ULYPX2010020 BK7 20.0x10.0 20.0 10.29 3.3 2 17.8
ULYPX2010025 BK7 20.0x10.0 25.0 12.87 3.0 2 23
ULYPX2020050 BK7 20.0x20.0 50.0 25.73 4.0 2 47.3
ULYPX2020075 BK7 20.0x20.0 75.0 38.6 3.3 2 72.8
ULYPX2020100 BK7 20.0x20.0 100.0 51.47 4.0 2 97.3
ULYPX2020150 BK7 20.0x20.0 150.0 77.2 3.7 3 147.5
ULYPX2020200 BK7 20.0x20.0 200.0 102.93 3.5 3 197.7
ULYPX2020250 BK7 20.0x20.0 250.0 128.67 3.3 3 247.7
ULYPX2020300 BK7 20.0x20.0 300.0 154.4 3.2 3 297.8
ULYPX2020500 BK7 20.0x20.0 500.0 257.33 4.0 3 497.9
ULYPX4020050 BK7 40.0x20.0 50.0 25.73 3.3 3 47.3
ULYPX4020075 BK7 40.0x20.0 75.0 38.6 3.3 2 72.8
ULYPX4020100 BK7 40.0x20.0 100.0 51.47 4.0 2 97.3
ULYPX4020150 BK7 40.0x20.0 150.0 77.2 3.7 3 147.5
ULYPX4020200 BK7 40.0x20.0 200.0 102.93 3.5 3 197.7
ULYPX4020250 BK7 40.0x20.0 250.0 128.67 3.4 3 247.7
ULYPX4020300 BK7 40.0x20.0 300.0 154.4 3.3 3 297.8
ULYPX4020500 BK7 40.0x20.0 500.0 257.33 3.2 3 497.9

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平凹方形柱面镜

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定制平凹圆型柱面镜
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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。

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。

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.



红外硅窗口片
硅窗口片
硅主要用作3至5微米波段的光学窗口片,并用作生产光学滤波器和窗口片的子系统。
激光等级镀金属反射镜
高功率激光反射镜

激光反射镜用于要求苛刻的激光应用中的光束控制。激光线反射镜是专为特定激光类型或波长设计的光学反射镜



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。



激光棱镜
激光等级棱镜
棱镜是透明的光学装置,其折射或反射光。 它们在激光技术中具有多种应用。
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。
菱形棱镜
高精度菱形棱镜

菱形棱镜的应用是在不影响图像方向的情况下控制和重定向光路。它们可以用来取代光学中心线的光束折叠和不同尺寸的立体系统.

熔融石英窗片
高精度紫外熔融石英窗片

熔融石英窗片具有低热膨胀性,在温度大幅改变、宽热工作范围和高激光损伤阈值下具有稳定性和抗热冲击性,,是从紫外到红外传输的更好选择。

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