| 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 |
| ALPAO标准变形镜变形镜,又称变形反射镜(DM),主要运用于各种自适应光学系统之中,主要用于校正波前畸变,它由很多驱动单元组合而成,每个驱动单元都有自己独立的控制器,在外加电压控制下,变形镜的镜面可以产生需要的形变量,从而对波前像差进行调制。变形镜是自适应光学系统中的重要部件之一 |
| CILAS的可变形反射镜CILAS的可变形反射镜,利用压电材料所有共享相同的属性(PZT)来工作的。他可以精确地控制很小的变形量(亚纳米级)和高响应速度(几百微秒)。 |
| IMRA公司 FCPA高能掺镱飞秒激光器FCPA μJewel系列掺镱飞秒光纤激光器是IMRA公司为工业应用量身定做的高功率FCPA系统。作为光纤激光器的开创和领军企业,IMRA在全球拥有超过150项专利技术,以向客户提供超过700台激光器,累计稳定运行时间达到百万小时。 |
| IMRA公司 Femtolite F/G/H系列掺铒拉曼频移飞秒光纤激光器产品描述Femtolite 是IMRA于2004年推出的飞秒光纤激光器,为1995年推出的全球首款商品光纤激光器的换代产品。Femtolite 已经出货数百台,其极低的失效和返修率令其它产品无法企及。 |
| | IMRA公司超快光纤激光器型号 AX-20 BX-60 FX-10 CX-20 \\r 中心波长(nm) 780 1560 800 780&1560 \\r 平均功率(mW) 20 60 10 20 \\r 脉宽(fs) 100 100 110 100 \\r 重复频率(MHz) 50 50 50 50 \\r Femtolite FX 系列 \\r 紧凑的激光头,尺寸:24.1×19.3×7.6cm |
| IMRA 超紧凑飞秒光纤激光器IMRA 是超快光纤激光器研发、制造和应用领域的世界领头羊。IMRA 通过国际先进思想交流,致力于未来工业应用关键技术的创意研究和创新发展。 IMRA飞秒光纤激光器主要应用于生物医学成像、双光子荧光激发、双光子聚合/三维激光光刻、多光子显微、非线性光谱学、泵探针实验、二次谐波成像、太赫兹产生和检测、超快计量、量子密码、微加工、医疗设备制造等众多领域。 |
| 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 |
| SID4 ElementADVANCED ADD-ON | for quantitative phase microscopy |
| 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-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 |
| 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 LWIRHIGH RESOLUTION PHASE & INTENSITY | in the far infrared region |
| SID4-eSWIRHIGH RESOLUTION EXTENDED SWIR WAVE FRONT SENSOR |
| SID4 SWIR-HRHIGH RESOLUTION + HIGH SENSITIVITY | for shortwave infrared |
| SID4 SWIRCOST-EFFECTIVE | HIGH RESOLUTION + HIGH SENSITIVITY |for shortwave infrared |
| SID4 NIRHIGH RESOLUTION PHASE & INTENSITY | at 1.55 µm |
| SID4HIGH RESOLUTION WAVEFRONT SENSOR | 400-1100 nm |
| SID4 UVCOST-EFFECTIVE UV WAVEFRONT SENSOR | High resolution (62 500 phase pixels) |
| SID4 V VacuumPhasics is innovating by proposing the first off-the-shelf vacuum compatible wavefront sensor on the market. The SID4 V is designed to perform wavefront measurements under high vacuum. the wavefront measurement is realized in-situ in the same condition as |
| Kaleo MTF Measurement StationPhasics innovative solution delivers the most complete lens characterization: off-axis MTF and wavefront error at multiple wavelengths. It benefits from Phasics patented technology to provide accurate results even for large Field of View (FoV). Kaleo MTF |