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| Holoeye空间光调制器 | ALPAO高速变形镜 | 波前分析仪Phasics | 自适应光学系统 | 数字微反射镜 DMD 数字微镜器件 | 光学元件器件DOE | 光刻仪 |
| 飞秒激光器 | 皮秒激光器 | 自相关仪 | 超短脉冲测量仪Frog | 超快激光器件 |
| 高功率连续波OPO | 高功率光纤激光器 | Qioptiq NANO 激光器 | 低噪声窄线宽激光器 | 可调谐激光器 | 半导体激光器和放大器 | SLD和ASE宽带光源 | 双波长输出氦氖激光器 |
| QIOPTIQ光纤耦合半导体激光器 | Diode & DPSS_qioptiq | 激光驱动白光光源 | 等离子体宽带光源 | 单色仪 | 光谱仪 | 光栅 | 辐射计 | 防嗮系数分析 | Optogma固体激光器 | Solarlight | 波长选择器 |
| 激光准直仪 | 红外激光观察镜 | 激光功率能量计 | 光学斩波器 | 光束质量分析仪 | 位敏探测器 | 红外相机 | O/E转换模块探测器 TIA-525S |
| 太赫兹相机及源 | 太赫兹探测器 | 太赫兹元器件及晶体 | 太赫兹光谱仪 | 太赫兹功率计 |
| Optiphase | 微光MOI |
| 普克尔盒/Pockels Cells | 电光调制器/Electro-Optics Modulators | 法拉第隔离器/Faraday Isolators | SESAM半导体可饱和吸收镜 | 探测器 | EOT高速光电探测器 | 其他未分类 |
| 电化学ECV 扩散浓度 | 接触电阻测量仪 | 四点探针测试仪 | 少子寿命测试仪 |
| 平行光管 |
| 光纤跳线及配件 | 无源器件 |
 | SID4 HRUNRIVALLED HIGH RESOLUTION | 400×300 phase pixels |
 | SID4 NIRHIGH RESOLUTION PHASE & INTENSITY | at 1.55 µm |
 | SID4 SWIRCOST-EFFECTIVE | HIGH RESOLUTION + HIGH SENSITIVITY |for shortwave infrared |
 | SID4 SWIR-HRHIGH RESOLUTION + HIGH SENSITIVITY | for shortwave infrared |
 | SID4-eSWIRHIGH RESOLUTION EXTENDED SWIR WAVE FRONT SENSOR |
 | SID4 LWIRHIGH RESOLUTION PHASE & INTENSITY | in the far infrared region |
 | SID4 DWIRPhasics introduces the first off-the-shelf high resolution wave front sensor for dual band infrared from 3 to 5 µm and 8 to 14 µm. The SID4 DWIR measures laser beam at 3.39µm and 10.6µm or source of any wavelength in between 3-5 µm and 8-14 µm such as bla |
 | SID4-sC8Designed for life science and material inspection microscopes, SID4-sC8 brings fast, accurate and truly quantitative phase measurement in a compact, plug-and-play solution. Biologists will benefit from label-free cell imaging, high sensitivity and automat |
 | SID4BioThe SID4Bio is a plug & play camera for quantitative phase imaging. It works with any microscope and enables measuring valuable numerical parameters on live cells. |
 | SID4 ElementADVANCED ADD-ON | for quantitative phase microscopy |
 | KaleoMultiWAVEThe Kaleo-MultiWAVE bench is a unique instrument that delivers wavefront error at multiple wavelengths. Optics such as lenses, filters or mirrors can be characterized at their working wavelength. The KaleoMultiWAVE works at different wavelengths to perfor |
 | IMRA掺铒800nm飞秒光纤激光器Femtolite系列F/G/HIMRA掺铒800nm飞秒光纤激光器Femtolite系列F/G/H IMRA的Raman-shifted拉曼位移技术，在810 nm的独特波长下拥有干净的脉冲形状和光谱，这使Femtolite可成为普遍存在的Ti：Sapphire激光器的优秀替代品。超紧凑稳定设计使得Femtolite飞秒激光器可应用于临床和工业环境。自2005年推出以来，Femtolite已得到广泛应用功率可达150mW@810nm/200mW@1620nm。目标应用包括太赫兹产生和探测、多光子荧光显微和二次谐波成像等 |
 | KaleoMTF for R&DThe KaleoMTF bench performs automated off-axis MTF and wavefront error measurements at multiple wavelengths. It also measures aberrations (Zernike coefficients), through focus MTF, distortion, EFL… All results are given in the lens exit pupil for accurate |
 | Kaleo IRPhasics bench makes infrared lens quality control very simple. IR MTF is obtained in a single shot at all frequencies with no need for scanning or complex alignment. All wavefront aberrations are also provided with this single acquisition. The Kaleo IR Be |
 | Kaleo iThe Kaleo-I instrument is especially designed for the quality control of refractive intraocular lens, whether spherical, aspheric, toric or bifocal. It achieves fast and reliable measurements thanks to the integration of our high resolution wavefront sens |
 | Lyncee Tec MEMS全息测振分析仪Lyncee Tec MEMS全息测振分析仪 全息MEMS测振分析仪记录MEMS振动周期中的三维形貌时序图，为MEMS振动测量提供了 的丰富数据，特别是可以在被测视场内任意一点测量面内和面外振幅（位移）及频率响应，这些独特优势与完善的配套软、硬件一起提供了一套完整的MEMS振动测量解决方案。 |
 | Lyncee Tec 时间分辨动态轮廓仪Lyncee Tec 时间分辨动态轮廓仪 数字全息显微镜 (DHM®) 为静态三维形貌测量提供干涉测量级的亚纳米分辨率。与此同时，得益于独特的非扫描全息技术，DHM®的图像抓取速率极短，最快可达1毫秒，这一 的4D测量能力为众多领域打开了广阔的应用空间。 |
 | Lyncee Tec Lens-Less sensor无透镜传感器LynceeLyncee Tec Lens-Less sensor无透镜传感器 Tec Lens-Less sensor无透镜传感器 |
| | PicoTwist单分子操纵磁镊装置PicoTwist单分子操纵磁镊装置 相对于传统的单分子操纵技术—微针、原子力显微术、光镊等存在作用力小且不易测量、实验环境受限制、对生物样品有损害等诸多不足。作为克服这些不足而出现的磁镊技术，具有作用力大、应用范围广、无损耗、稳定等优势，很好得解决了这些问题。磁镊提供的作用力在大小内可调，既可从分子外部进行操作，也可以深入细胞内部，还可对溶液体系中的鲜活样品进行操作. |
 | 美国Optofluidic品牌nanotweezer微流控纳米拉曼光镊(NanoTweezer Raman)美国Optofluidic品牌nanotweezer微流控纳米拉曼光镊(NanoTweezer Raman) |