看了激光产品的用户又看了
TiF-Kit飞秒激光器自组装工具箱
产品介绍:
TiF-Kit是一套光学和机械组件工具箱,包含飞秒固体激光器的所有重要组件,并且可以根据用户要求进行自定义配置。
与TiF系列激光器相比,该组装工具箱是一个更简单的方案,并且可以根据客户要求提供各种自定义配置。该系统使用一台532 nm DPSS激光器进行泵浦。系统的输出功率取决于泵浦功率。
系统组成:
基本组成部分: - 刚性光学元件 - 介电超快腔镜 - 泵浦光束控制和聚焦光学元件 - 钛蓝宝石晶体,带有可调底座和冷却通气口 - 手动棱镜和调谐狭缝 - 用于锁模启动的手动启动器 | 可选配件: - 机箱外壳 - 热稳定主板 - 泵浦激光器冷却适配器 - USB调谐狭缝控制软件 - 脉冲序列输出自动启动器 - 手动或电动CW调谐组件 - CW标准具 |
产品特点:
2 成本低,高性价比
2 灵活的布局和可选的配件
2 输出功率最高可达1.5 W
技术参数:
型号 | TiF-Kit-15 | TiF-Kit-50 | TiF-Kit-100 | CrF-Kit 65 |
脉宽 | <15-30* fs | <50 fs | <100 fs | <65 fs |
调谐范围** | 780-840 nm | 740-950 nm | 715-980 nm | 1240-1270 nm |
输出功率** | 200-500 mW | 100 mW - 1 W | 100 mW - 1.5 W | 100-250 mW |
最大泵浦功率 | 3-6 W | 2-10 W | 2-10 W | 10-15 W |
偏振 | 线性,水平 | |||
空间模式 | TEM00 | |||
重复频率 | 70-95 MHz (固定) | |||
* - 带有外部群速度色散补偿; ** - 取决于泵浦功率和工作温度(例如715-980nm范围内,泵浦功率为10W)。 |
用户单位 | 采购时间 |
---|---|
电子科技大学 | 2016-05-10 |
帝尔时代(天津)科技有限公司 | 2017-01-08 |
东莞市春和电子商贸有限公司 | 2015-11-14 |
上海交通大学 | 2016-03-08 |
上海交通大学 | 2014-09-24 |
保修期: 1年
是否可延长保修期: 否
现场技术咨询: 无
免费培训: 1
免费仪器保养: 1
保内维修承诺: 1
报修承诺: 1
Avesta TeMa掺镱固体飞秒激光器
型号:TeMa 5万Avesta TiF-15钛:蓝宝石飞秒激光器
型号:TiF-15 5万Avesta TiF-50型 钛:蓝宝石飞秒激光器
型号:TiF-50 5万Avesta TiF-100型 钛:蓝宝石飞秒激光器
型号:TiF-100 5万Van der Waals coupling is emerging as a powerful method to engineer physical properties of atomically thin two-dimensional materials. In coupled graphene–graphene and graphene–boron nitride layers, interesting physical phenomena ranging from Fermi velocity renormalization to Hofstadter’s butterfly pattern have been demonstrated. Atomically thin transition metal dichalcogenides, another family of two-dimensional-layered semiconductors, can show distinct coupling phenomena. Here we demonstrate the evolution of interlayer coupling with twist angles in as-grown molybdenum disulfide bilayers. We find that the indirect bandgap size varies appreciably with the stacking configuration: it shows the largest redshift for AA- and AB-stacked bilayers, and a significantly smaller but constant redshift for all other twist angles.
We report on the generation of broadband, high-energy femtosecond pulses centered at 1.28 μm by stimulated Raman scattering in a pressurized hydrogen cell. Stimulated Raman scattering is performed by two chirped and delayed pulses originating from a multi-mJ Ti:sapphire amplifier.The Stokes pulse carries record-high energy of 4.4 mJ and is recompressed down to 66 fs by a reflective grating pair. We characterized the short-wavelength mid-infrared source in view of energy stability, beam profile, and conversion efficiency at repetition rates of 100 and 10 Hz. The demonstrated high-energy frequency shifter will benefit intense THz sources based on highly nonlinear organic crystals.
A high-stability and high-efficiency ring Ti:sapphire regenerative amplifier is demonstrated based on a double-gating pulse picker at a repetition rate of 1 kHz. Pulse energy up to 5.7 mJ is obtained using a pump energy of 20.0 mJ at 527 nm, corresponding to a relatively high slope efficiency of 30.3%. After a grating compressor, the laser pulse is compressed to 37.2 fs with an energy of 4.1 mJ. The beam quality factors M2 are 1.4 and 1.3 in tangential and sagittal directions, respectively. The measured root mean square energy stability is better than 0.31% over an 11 h period.
阿维斯塔激光产品TiF-Kit的工作原理介绍
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