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基于LiF∶F2晶体在近红外飞秒脉冲激光作用下产生F2色心向F3 色心的转变,以及两种色心荧光光谱的不同,实现了荧光反射共焦读出和多光子写入的三维光数据存储的原理性实验.钛宝石再生放大器输出的脉冲宽度100fs、中心波长800nm、重复频率1kHz的超短脉冲激光束,用数值孔径0.68的显微物镜聚焦到LiF:F2晶体内部,通过移动晶体实现了三维逐位式数据写入;用405nm的连续蓝光激发存储位,通过探测F3 色心产生的540nm荧光,实现了对信息位进行快速非破坏性的反射共焦读出.与多光子三维存储的透射共焦散射读出和相衬读出相比,格式与现存光盘技术兼容,结构简单;更重要的是,存储信息位是依靠荧光光谱的变化,折射率变化很小,可以有效增加读出层数. 相似文献
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We report the generation of ultrashort pulses in ytterbium-doped fibre oscillator emitting around 1.05μm at a repetition rate of 17.6 MHz. A diode laser with single silica fibre at 976nm pumps the ytterbium fibre laser, the all-fibre picosecond pulsed oscillator has excellent stability and compact size, and freedom from misalignment. After amplifying, pulse energy of 3.4 nJ and an average power of 60 m W are obtained. The compression is obtained with a grating pair out of the cavity. The compressor produces 307fs with the peak power 5.47kW. A practical fibre-based source with good performance is thus demonstrated. 相似文献
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基于传输速率方程,对Ho3+:ZBLAN光纤激光器的动态特性--上能级粒子数以及输出激光功率的弛豫振荡特性进行了数值分析.通过忽略光纤参数对传输方向的依赖性,抽运光和信号光的功率传输方程被分别简化处理.结果表明,在5I6能级的粒子数首先经历一次弛豫振荡后,5I6和5I7能级的粒子数交替弛豫振荡并达到稳态;同样,在3μm波长的激光功率首先经历一次弛豫振荡后,3μm和2μm波长的激光功率交替弛豫振荡并达到稳态,而且,弛豫振荡时的峰值功率远大于稳态时的激光功率. 相似文献
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本文报道了以1313nmNd:YLF激光脉冲泵浦掺饵(Er3+)单模GeO2/SiO2光纤而产生多波长可见光的实验,在该光纤中观察到(463~510)nm间的多波长放大自发辐射过程,此过程对应于Er3+离子的2G7/2等几个激发态到4I13/2亚稳态的跃迁.其激发过程是分步的四光子吸收过程,同时,掺饵光纤的红外发射峰1530nm(4I13/2-4I15/2)与1313nm泵浦光之间的三波混频过程也对这一区间的连续多峰的光谱结构有贡献.实验中还观察到540nm附近的绿光辐射. 相似文献
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GENERATION OF MULTI-WAVELENGTH VISIBLE LIGHT IN Er3+-DOPED AND Er3+/Yb3+-DOPED SINGLE-MODE OPTICAL FIBER PUMPED AT 1313 nm 下载免费PDF全文
We report the generation of multi-wavelength visible light through amplified spontaneous emission (ASE) in Er3+-doped and Er3+/Yb3+-doped germanosilicate single-mode optical fiber pumped by a Nd:YLF laser at 1313nm. In the Er3+-doped fiber, the intense multi-wavelength blue emission hnes around 463-510nm corre-spond to transitions born 2G7/2 etc. excited states to the metastable 4I13/2 state, and their pumping mechanists is aecomphshed by a stepwise four-photon absorption. Some emission hnes in this wavelength region are attributed to the three-wave sum-frequency process of 1313 and 1530nm (corresponds to 4I13/2 -4I15/2). The intense green emission hnes at 525 and 540 nm are also observed in the Er3+-doped fiber. In the Er3+/Yb3+-doped fiber the blue and green lines are very weak compared with those in the Er3+-doped fiber. 相似文献
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