产品
Home /

滤光片

/光学玻璃中性密度滤光片

光学玻璃中性密度滤光片

中性密度滤光片让摄影师非常容易地控制图像中的曝光。该滤光片阻止光线到达相机传感器,因此我们可以让相机在更长的时间内保持更大的通光孔径。
  • 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的中性密度滤光片是一种可以均匀地降低或改变所有波长或颜色强度,但不会改变颜色色调的滤光片。



1. 什么是中性密度滤光片?


中性密度滤光片让摄影师非常容易地控制图像中的曝光。该滤光片阻止光线到达相机传感器,因此我们可以让相机在更长的时间内保持更大的通光孔径。


2. 中性密度滤光片的用途是什么?


标准摄影中性密度滤光片的目的是减少光量进入镜头。这样做允许摄影师选择光圈,曝光时间和传感器灵敏度的组合,否则会产生过度曝光的图像。



常用规格


尺寸公差:±0.5mm

表面质量:80-50或更高

表面面型:4-6λ或更好

涂层:可选




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
强脉冲滤光片
IPL滤光片

IPL滤光片是IPL(强脉冲光)机器的关键光学元件,可阻挡紫外波,并为激光设备传输400nm1200nm的有用波,如光子嫩肤脱毛血管和痤疮治疗皮肤再生


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


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。


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。

BK7激光等级反射镜
激光等级反射镜

我司可提供带有特殊涂层的高损伤阈值的激光反射镜。

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。


色散棱镜
30° - 60° - 90°色散棱镜

色散棱镜用于需要将入射光分离成其组成波长的应用中。例如,当白光进入色散棱镜时,它被分成三个部分:红、绿和蓝。色散棱镜是理想的光谱学或激光调谐。

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.



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。

分光五角棱镜
镀氟化钙的分光五角棱镜

分光五角棱镜是通过在棱镜其中一个倾斜面上添加一个楔,并加上部分反射涂层,可以将五角棱镜用作分光镜,透过率/反射率(T/R)比为50/50,其他比例的分光五角棱镜也能根据您的要求定制。

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。
可见光镀增透消色差透镜
宽带增透膜消色差透镜

消色差透镜用来减小或消除色差。消色差透镜设计亦有助于减少球面像差。消色差透镜是一系列应用的理想选择,包括荧光显微镜、图像中继、检测或光谱学。消色差透镜通常是将两个元件胶合在一起或将两个元件安装在一个机械件中,它所产生的光斑尺寸比类似的单透镜要小。


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