产品
Home /

光学材料

/激光晶体

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。


立即查询
  • 描述
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
Optical color less glass
光学玻璃
光学玻璃可以改变光的方向,以及紫外光,可见光或红外光的相对光谱分布。光学玻璃材料是最常见的类型,因为它具有优异的光学性能,如高透光性和环境稳定性。
Colored Glass Substrates
有色玻璃(截至型,选择吸收型,中性密度型)

UNI Optics供应材料包括中性密度,短程,长通,带通,紫外线,红外线,吸热和色温转换滤光片。

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。
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.



BK7球透镜和半球透镜
融石英球透镜和半球透镜
球透镜通常用于改善光纤耦合应用中的信号质量,或用于内窥镜检查或条形码扫描应用。 球镜具有较短的后焦距,可最大限度地缩短球镜与光纤之间的距离。 Uni Optics在各种基材中提供各种球镜,可实现紫外到近红外光谱的性能。
氟化钙窗片
氟化钙窗片

氟化钙窗片及透镜用于紫外和红外光谱。根据客户的要求定制CaF2CaF2透镜和楔角片以及直径220毫米以上CaF2


装配的长波通滤镜
长波通滤镜

长波通滤光片适用于各种应用,如气体监测,温度,传感,热成像和运动传感等。长波通滤光片可阻挡较短波长并传输较长波长。 阻挡可以来自反射,吸收或组合。 带通中的透射可以通过第二表面上的增透膜涂层来增强。


激光透镜
激光等级透镜

激光透镜用于在各种激光应用中聚焦来自激光束的准直光。激光透镜包括一系列透镜类型,包括平凸透镜,激光划线透镜或激光发生器透镜。 激光头设计用于根据透镜类型以几种不同的方式聚焦光线,例如聚焦到一个点,一条线或一个环。许多不同的镜头类型可用于各种波长。

偏振分光棱镜
偏振分光棱镜

偏振分光棱镜由两个直角棱镜胶合而成,其中一个棱镜的斜面镀有偏振介质膜。当与正常入射、非偏振光一起使用时,入射光被分成两束偏振光,P偏振光可直接穿过,S偏振光以90°角反射出来。

微型元件锥透镜
3mm直径镀铝膜锥透镜

锥形透镜是圆柱形棒透镜,其一端加工成锥形表面。 通常研磨杆的圆周,而抛光锥形表面。

有色玻璃窗片
镀增透膜有色玻璃窗片
有色玻璃改变了光辐射的光谱特性。 因此,它们允许在需要改变的情况下进行科学实验和工业应用。 您可以将彩色玻璃滤镜组合在一起以更改带通或增加衰减。
喷黑漆角锥
N-BK7角锥棱镜

角锥棱镜又称反射它有三个相互垂直的表面和一个斜边面。通过斜边进入的光依次被三个表面反射,并通过平行于入射光束的斜边面出现,而不考虑入射光束的方向由于其特殊的性能,常被用于距离测量、光学信号处理和激光等领域。

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