- CryLaS GmbH
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- ID Photonics GmbH
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- PhotoMachining
- Photon Energy GmbH
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- PhotoScribe Technologies Inc.
- PicoQuant
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- PolarOnyx
- Power Technology Inc.
- PPI Systems
- Polaris Motion
- Precitec
- Prima Power Laserdyne LLC
- Radian Laser Systems
- RAM Photonics LLC
- Rayscience Optoelectronics Innovations Co Ltd
- ScannerMax
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- Shanghai HXF-LaiYi
- SI Engineering GmbH
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- SIOS Messtechnik GmbH
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- STC Catalysts Inc
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- Synrad - A Novanta Company
- Thinklaser
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- ULT AG
- VPIphotonics
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- WL Photonics Inc.
- ZENNA Laser Solutions BV
- Laserse Inc.
- Wisely Laser Machinery Limited
- Suzhou Yosoon Laser Equipment Co., Ltd
- Optizone Technology
- Suzhou Delphi Laser Co., Ltd
- Nanjing Metalaser Photonics Co.,Ltd.
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- APE Angewandte Physik & Elektronik GmbH
- Areté Associates
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- Clark-MXR, Inc
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- CryLaS GmbH
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- Dausinger + Giesen
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- IDIL Fibres Optiques
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- Kimmon Koha
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- Neptec Optical Solutions
- MKS | Newport
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- NP Photonics, Inc.
- NUBURU
- Nuphoton Technologies, Inc.
- O.R. Lasertechnology
- OCTLIGHT
- Omicron-Laserage
- OPELUS Technology Corporation
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- Photonics Industries
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- Picotronic
- Powerlase Limited
- Precision Laser Scanning, LLC
- Precision Micro-Optics
- ProPhotonix
- Q-Peak
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- Quantifi Photonics
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- Quantum Light Instruments
- R&D Ultrafast Lasers
- Radiant Dyes Laser
- Radiantis
- RAM Photonics
- Ray Technologies
- Redfern Integrated Optics
- Research Electro-Optics, Inc.
- Ricoh Company, Ltd.
- RMI Laser, LLC
- Roithner Lasertechnik
- RPMC Lasers Inc.
- Sacher Lasertechnik
- Santec Corporation
- SCANLAB AG
- Sepradel
- Sintec Optronics
- Sirah Lasertechnik
- SOL Instruments
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- Soliton Laser und Messtechnik GmbH
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- Symphotic TII Corporation
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- Thales Group
- The Optoelectronics Company Ltd
- 索雷博
- TOPTICA Photonics
- Trimedyne, Inc
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- Skylark Lasers
- Unilase Ltd
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- UVC Photonics
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- Wavelength Opto-Electronic
- Wavelength References
- WORKSHOP OF PHOTONICS
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- Cymer
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- VI Systems GmbH
- Optowell
- Pure Photonics
- BluGlass Limited
- 朗研光电
- Altos Photonics, Inc.
- Purex International Ltd
- QGLex Inc
- ALTER
- Leonardo DRS
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Skylark 780 NX CW C-DPSS激光器
厂家:Skylark Lasers
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Skylark 640 NX C-DPSS激光器
厂家:Skylark Lasers
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Skylark 532 NX C-DPSS激光器
厂家:Skylark Lasers
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Skylark 349 NX CW C-DPSS紫外激光器
厂家:Skylark Lasers
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Skylark 320 NX CW C-DPSS紫外激光器
厂家:Skylark Lasers
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ASE-C-80系列 3通道ASE光源台式设备器
厂家:Optilab
光电查为您提供77个产品。下载资料,获取报价,实现功能、价格及供应的优化选择。
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波长: 213nm 平均值功率: 0.02W 重复频率: 0 - 1 kHz 空间模式: 1 脉宽: 1ns
新的E-MOPA激光器系列基于二极管泵浦的被动调Q Nd:YAG激光器(主振荡器),该激光器由二极管泵浦的光放大器(功率放大器)组合而成。通过这种MOPA技术,与非放大系统相比,可以获得恒定且光学稳定的更高脉冲能量和平均功率。通过使用高纯度非线性晶体,集成倍频和和频转换允许将波长下滚到532、355或266nm。提供脉冲能量高达200µJ、平均功率高达200mW的各种型号。脉冲频率由外部或内部触发,单次触发频率高达1kHz。由于微芯片的设计,在1ns的脉冲长度范围内达到了高达200kW的峰值功率。激光器结构紧凑,坚固耐用,易于集成到仪器和计量设备中。
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波长: 266nm 平均值功率: 0.04W 重复频率: 0 - 1 kHz 空间模式: 1 脉宽: 1ns
新的E-MOPA激光器系列基于二极管泵浦的被动调Q Nd:YAG激光器(主振荡器),该激光器由二极管泵浦的光放大器(功率放大器)组合而成。通过这种MOPA技术,与非放大系统相比,可以恒定地和光学稳定地获得更高的脉冲能量和平均功率。通过使用高纯度非线性晶体,集成倍频和和频转换允许将波长下滚到532、355或266nm。提供脉冲能量高达200µJ、平均功率高达200mW的各种型号。脉冲频率由外部或内部触发,单次触发频率高达1kHz。由于微芯片的设计,在1ns的脉冲长度范围内达到了高达200kW的峰值功率。激光器结构紧凑,坚固耐用,易于集成到仪器和计量设备中。
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波长: 355nm 平均值功率: 0.1W 重复频率: 0 - 1 kHz 空间模式: 1 脉宽: 1ns
新的E-MOPA激光器系列基于二极管泵浦的被动调Q Nd:YAG激光器(主振荡器),该激光器由二极管泵浦的光放大器(功率放大器)组合而成。通过这种MOPA技术,与非放大系统相比,可以获得恒定且光学稳定的更高脉冲能量和平均功率。通过使用高纯度非线性晶体,集成倍频和和频转换允许将波长下滚到532、355或266nm。提供脉冲能量高达200µJ、平均功率高达200mW的各种型号。脉冲频率由外部或内部触发,单次触发频率高达1kHz。由于微芯片的设计,在1ns的脉冲长度范围内达到了高达200kW的峰值功率。激光器结构紧凑,坚固耐用,易于集成到仪器和计量设备中。
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波长: 532nm 平均值功率: 0.2W 重复频率: 0 - 1 kHz 空间模式: 1 脉宽: 1ns
新的E-MOPA激光器系列基于二极管泵浦的被动调Q Nd:YAG激光器(主振荡器),该激光器由二极管泵浦的光放大器(功率放大器)组合而成。通过这种MOPA技术,与非放大系统相比,可以恒定地和光学稳定地获得更高的脉冲能量和平均功率。通过使用高纯度非线性晶体,集成倍频和和频转换允许将波长下滚到532、355或266nm。提供脉冲能量高达200µJ、平均功率高达200mW的各种型号。脉冲频率由外部或内部触发,单次触发频率高达1kHz。由于微芯片的设计,在1ns的脉冲长度范围内达到了高达200kW的峰值功率。激光器结构紧凑,坚固耐用,易于集成到仪器和计量设备中。
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波长: 266nm 最大输出功率: 100mW 运行模式: CW
DPSS CW深紫外激光器系列FQCW-266配有谐振频率转换级,发射266 nm的固定波长。激光头包含在密封的铝制外壳中,可在各种环境条件下工作。激光头的散热是通过空气对流完成的,不需要其他设备(冷却器、风扇等)。FQCW266系列DPSS CW深紫外激光器在266nm单频工作时输出功率高达500 MW。与其他266nm连续激光器相比,FQCW266系统具有超过1000m的长相干长度、窄线宽(300kHz)、低功耗和小尺寸。FQCW-266即插即用激光器带有一个控制单元,允许通过串行(RS232 USB)接口进行按钮控制或远程控制操作。激光器提供了极好的光束质量,M2低于1.3,光束发散度低于0.8 mrad(全角),低强度噪声低于0.5%RMS(100 kHz-10 MHz)和良好的功率稳定性(8小时内1%)。这些CW激光单元是拉曼光谱、晶片检测和光致发光等需要长相干长度的应用的合适工具。这些紫外连续波激光器提供出色的光束质量和性能,旨在满足工业应用和密集研发的挑战性要求。
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波长: 266nm 最大输出功率: 500mW 运行模式: CW
DPSS CW深紫外激光器系列FQCW-266配有谐振频率转换级,发射266nm的固定波长。激光头包含在密封的铝制外壳中,可在各种环境条件下工作。激光头的散热是通过空气对流完成的,不需要其他设备(冷却器、风扇等)。FQCW266系列DPSS CW深紫外激光器在单频操作中在266 nm处提供高达500 MW的功率。与其他266nm连续激光器相比,FQCW266系统具有超过1000m的长相干长度、窄线宽(该激光器提供了优异的光束质量,M2低于1.3,光束发散度低于0.8mrad(全角),低强度噪声低于0.5%RMS(100kHz-10MHz)和良好的功率稳定性(8小时1%)。这些CW激光单元是拉曼光谱、晶片检测和光致发光等需要长相干长度的应用的合适工具。这些紫外连续波激光器提供出色的光束质量和性能,旨在满足工业应用和密集研发的挑战性要求。
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波长: 266nm 最大输出功率: 200mW 运行模式: CW
DPSS CW深紫外激光器系列FQCW-266配有谐振频率转换级,发射266 nm的固定波长。激光头包含在密封的铝制外壳中,可在各种环境条件下工作。激光头的散热是通过空气对流完成的,不需要其他设备(冷却器、风扇等)。FQCW266系列DPSS CW深紫外激光器在266nm单频工作时输出功率高达500 MW。与其他266nm连续激光器相比,FQCW266系统具有超过1000m的长相干长度、窄线宽(300kHz)、低功耗和小尺寸。FQCW-266即插即用激光器带有一个控制单元,允许通过串行(RS232 USB)接口进行按钮控制或远程控制操作。该激光器提供了极好的光束质量,M2低于1.3,光束发散度低于0.8 mrad(全角),低强度噪声低于0.5%RMS(100 kHz-10 MHz)和良好的功率稳定性(8小时1%)。这些CW激光单元是拉曼光谱、晶片检测和光致发光等需要长相干长度的应用的合适工具。这些紫外连续波激光器提供出色的光束质量和性能,旨在满足工业应用和密集研发的挑战性要求。