二倍频泵

飞秒激光器FFL系列卓立汉光自主研发的全新一代高功率、高能量飞秒激光器。以原有的光纤种子源技术为基础，加上固体放大技术，使单脉冲能量可达500μJ或更高。同时，脉冲宽度在600fs以内，保证加工效果，降低热影响区。作为具有CPA结构的高功率工业飞秒激光器， FFL系列专为24×7的长时间运行而设计，稳定性高，适合需要高能量脉冲的各类工业领域与科研应用。 FFL-25高能量飞秒激光器应用场景 &bull 玻璃切割&bull 非线性研究&bull 微加工等领域FFL-25高能量飞秒激光器产品特性&bull 可靠的放大技术,支持高脉冲能量输出&bull 支持脉冲宽度可调&bull 支持脉冲编辑POD与Burst Mode&bull 可选二倍频/三倍频/三波段模块&bull 紧凑的机械与工业设计，适用于各类光学平台或设备内部 规格参数参数FFL 25 双波长中心波长1030±5nm515±3nm平均功率＞ 20W＞ 2.5W脉冲宽度600fs -10ps 可调600fs -10ps 可调重复频率单脉冲 -1MHz 可调单脉冲 -1MHz 可调单脉冲能量＞ 200 µ J @ 100kHz＞ 25 µ J @ 100kHz输出方式空间光输出空间光输出消光比100：1100：1光束指向稳定性 25 urad 25 urad功率稳定性0.5% rms0.5% rms光束质量M2 1.3M2 1.3发散角 1mrad 1mrad尺寸（- 体机）750×500×156 mm210×500×93 mm危险4级激光辐射 避免眼睛或皮肤受到直射或散射

1X0二倍频模组（5W 532nm）1x0 High Power SHG Mixer产品特色： 即插即用 单通道&高效率 紧凑&稳固 光纤输入，自由空间光输出产品参数：

倍频器 ASG， ATSG，AFsG和AMG二倍频模块（三倍频、四倍频）的功能是通过倍频转换输入波长。输入波长可以从720nm -1600nm，工作原理是利用倍频技术产生稳定的激光源，在飞秒量级的应用中具有较好光束质量和优秀的脉冲扩展。 产品特色：高转换效率小离散角小光束发散角不发热 产品一览表：产品型号输入波长范围二倍频输出三倍频输出四倍频输出转换效率ASG720-1600 nm360-800 nmnonoSH: 20-50%ATsG750-1600 nm375-800 nm250-533 nmnoSH: 20-50% TH: 3-15%AFsG820-1600 nm410-800 nmno205-400 nmSH: 20-50% FH: 3-10%AMG780-1600 nm390-800 nm260-533 nm195-400 nmSH: 30-60% TH: 5-10% FH: 1-10% 产品详细参数详情：ASG. 二倍频器二倍频用于上转换（倍频）飞秒激光源的固有频率。ASG-O(for oscillators)ASG-A(for amplifiers)可实现的输入波长范围*720-1600 nm输入波长调谐范围**50-100 nm输出波长***360-800 nm输入脉宽20 fs输入偏振linear, horizontal输出偏振linear, vertical输入平均功率0.1-3 W10 W输入脉冲能量2 uJ2 uJ - 10 mJ输入光斑直径1/е^22 mm10 mm转换效率****20-50%30-50%脉冲展宽100 fs尺寸280x140x190 mm* - may be covered by several exchangeable optics sets, please indicate the desired wavelength range upon your request ** - typical with one optics set, depends on exact central wavelength and pulse duration *** - defined by input wavelength **** - defined by input pulse energy and input pulse duration. ATsG.二倍频、三倍频器（用于飞秒激光）ATsG-O(for oscillators)ATsG-A(for amplifiers)可实现的输入波长范围*750-1600 nm输入波长调谐范围**50-100 nm输出波长***375-800 nm (SH)250-533 nm (TH)输入脉宽20 fs输入偏振linear, horizontal输入平均功率0.3-3 W10 W输入脉冲能量2 uJ2 uJ - 10 mJ输入光斑直径1/е^22 mm10 mm转换效率****20-50% (SH)3-8% (TH)30-50% (SH)8-15% (TH)脉冲展宽100 fs (SH)200 fs (TH)100 fs (SH)180 fs (TH)输出偏振SH - linear, vertical ТГ - linear, horizontal尺寸480x222x192 mm* - may be covered by several exchangeable optics sets, please indicate the desired wavelength range upon your request ** - typical with one optics set, depends on exact central wavelength and pulse duration *** - defined by input wavelength **** - defined by input pulse energy and input pulse duration. AFsG. 二倍频、四倍频器（用于超快激光）AFsG-A-1045 二倍频和四倍频用于Yb-Doped 固态和光纤放大系统AFsG-O(for oscillators)AFsG-A(for amplifiers)可实现的输入波长范围*820-1600 nm输入波长调谐范围**50-100 nm输出波长***410-800 nm (SH)205-400 nm (FH)输入脉宽50 fs输入偏振linear, horizontal输入平均功率0.3-3 W10 W输入脉冲能量2 uJ2 uJ - 10 mJ输入光斑直径1/е^22 mm8 mm转换效率****20-50% (SH)3-8% (FH)30-50% (SH)5-10% (FH)脉冲展宽100 fs (SH), 1000 fs (FH)输出偏振SH - linear, vertical FH - linear, horizontal尺寸480x222x192 mm* - may be covered by several exchangeable optics sets, please indicate the desired wavelength range upon your request ** - typical with one optics set, depends on exact central wavelength and pulse duration *** - defined by input wavelength **** - defined by input pulse energy and input pulse duration. AMG.二倍频、三倍频、四倍频模块AMG-A-1030多倍频器用于1um放大器AMG-A(for amplifiers)可实现的输入波长范围*780-1600 nm输入波长调谐范围**50-100 nm输出波长***390-800 nm (SH)260-533 nm (TH)195-400 nm (SH)输入脉宽50 fs输入偏振linear, horizontal输入平均功率10 W输入脉冲能量0.2-10 mJ输入光斑直径1/е^28 mm转换效率****30-50% (SH), 5-10% (TH), 1-10% (FH)脉冲展宽100 fs (SH), 250 fs (TH), 1000 fs (FH)输出偏振linear: SH - vertical TH - horizontal FH - vertical尺寸480x222x192 mm* - may be covered by several exchangeable optics sets, please indicate the desired wavelength range upon your request ** - typical with one optics set, depends on exact central wavelength and pulse duration *** - defined by input wavelength **** - defined by input pulse energy and input pulse duration.