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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。
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400nm至1200nm的有用波，如光子嫩肤脱毛、血管和痤疮治疗、皮肤再生。
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1，什么是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400nm至1200nm的有用波。
2，IPL滤光片有哪些应用？
IPL滤光片适用于各种应用，如IPL机器，IPL设备，光子嫩肤，脱毛，血管和痤疮治疗以及皮肤再生。
3，优恩立光电可以提供哪些波长？
优恩立光电可提供不同波长的IPL滤光片，包括495,515,550,560,570,590,615,645,695,755,780 nm和1200nm。其他波长可根据要求提供。
通用规格：
|
基底材料 |
N-BK7，B270，熔融石英或其他 |
|
尺寸公差 |
±0.1（通用精度），±0.01（高精度） |
|
厚度公差 |
±0.2（通用精度），0.005（高精度） |
|
表面质量 |
60/40（通用精度），20/10（高精度） |
|
通光孔径 |
> 80％（一般精度），95％（高精度） |
|
平行度 |
<3弧分（通用精度）， <5弧秒（高精度） |
|
面型 |
<λ/ 2 @ 633nm（通用精度）， <λ/ 10 @ 633nm（高精度） |
|
波长范围 |
300〜1200nm的 |
|
通带平均透过率 |
> 90％的 |
|
拒绝带平均透过率 |
≤0.5％ |
|
入射角 |
0° |
|
倒角 |
0.2〜0.4mm×45° |
|
可用波长 |
515〜1200,530〜1200,550〜1200,560〜1200, 570〜1200,590〜1200,615〜1200, 645〜1200,695〜1200,755〜1200,780〜1200nm |
典型的波长传输数据
上一个 :
机器视觉带通滤光片
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。
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。
镀宽带增透膜的斜边直角棱镜
直角棱镜通常用于改变光路，或用于将光束重新定向90°。直角棱镜是设计成90°角的棱镜，根据棱镜的方向产生倒置或反转的左手图像，同时使用两个直角棱镜是理想的使图像或光束位移的应用。这些棱镜也被称为镜像反射棱镜。
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。
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.
MgF2镀膜双凸透镜
融石英球透镜和半球透镜
