一种420兆赫的Cr:forsterite飞秒环形激光器及其在1-2微米范围内连续生成的应用

I. Thomann, S. Diddams, A. Bartels, K. L. Corwin, N. Newbury, L. Hollberg, J. Nicholson, M. Yan
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引用次数: 2

摘要

我们提出了一种以420 MHz重复频率产生30 fs脉冲的Cr:forsterite环形激光器。输出宽在高度非线性光纤产生光谱覆盖1050- 2200nm。美国光学学会OCIS编码:(060.45 10)光通信,(140.7090)超快激光器,(120.3940)计量学我们已经开发了一种掺铬的forsterite飞秒环形激光器,它以420 ME-Iz的重复率产生30 fs脉冲,平均功率为-500 mW。据我们所知,这是第一个环形结构,也是迄今为止报道的飞秒Cr:forsterite激光器的最高重复率。紧凑的固态设计和广谱输出使该激光器在重要的1.3-1.6 pm范围内的应用具有吸引力。在高度非线性光纤中,激光输出的额外光谱展宽导致超连续谱的产生,最宽的光谱跨越一个八度程。潜在的光学频率梳可以连接到现有的光学频率标准,从而在近红外光谱中建立一个广泛的精确已知频率阵列。由于其对光纤通信的重要性[1],1.3-1.6 pm范围是传播飞秒激光频率测量新工具的自然方向[2-41]。为此,我们研制了高重复率、宽带Cr:forsterite飞秒激光器。我们的激光器由一个紧凑的,无棱柱的6镜环形腔组成,类似于早期使用Tksapphire[5]的工作。目前配置的重复频率是420 MHz,但我们相信它可以很容易地增加到1 GHz。泵浦是一个10w的镱光纤激光器,工作在1075nm。腔内色散补偿由啁啾和GTI(光栅- tournois干涉仪)镜的组合提供。为了获得最佳色散补偿,我们获得了59 nm的FWHM谱宽。该光谱如图1 (a)中的曲线(iv)所示。外部压缩啁啾镜提供30秒脉冲。平均功率为480 mW,意味着脉冲能量为1.1 nJ。One hundred.
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A 420 MHz Cr:forsterite femtosecond ring laser and its use for continuum generation in the 1-2 micron range
We present a Cr:forsterite ring laser producing 30 fs pulses at a 420 MHz repetition rate. The output is broadened in highly nonlinear fiber yielding spectra covering 1050-2200 nm. 02000 Optical Society of America OCIS codes: (060.45 10) Optical communications, (140.7090) Ultrafast lasers, (120.3940) Metrology We have developed a chromium-doped forsterite femtosecond ring laser that generates 30 fs pulses at a 420 ME-Iz repetition rate with -500 mW of average power. To our knowledge, this is the first ring configuration as well as the highest repetition rate yet reported for a femtosecond Cr:forsterite laser. The compact solid-state design and broad spectral output make this laser attractive for applications in the important 1.3-1.6 pm regime. Additional spectral broadening of the laser output in highly nonlinear optical fibers leads to supercontinuum generation, with the broadest spectra extending across an octave. The underlying optical frequency comb can be linked to existing optical frequency standards, thereby establishing a broad array of precisely known frequencies across the near infrared spectrum. Because of its importance for fiber-based communications [l], the 1.3-1.6 pm regime is a natural direction in whch to spread the new tools of femtosecond-laser-based frequency metrology [2-41. Towards this end, we have developed a high repetition rate, broadband Cr:forsterite femtosecond laser. Our laser consists of a compact, prismless 6-mirror ring cavity similar to earlier work with Tksapphire [5]. The repetition rate in this present configuration is 420 MHz, yet we believe it could readily be increased to 1 GHz. The pump is a 10 W Ytterbium fiber laser operating at 1075 nm. Intra-cavity dispersion compensation is provided by a combination of chirped and GTI (Gires-Tournois interferometer) mirrors. For the optimal dispersion compensation, we obtain a FWHM spectral width of 59 nm. This spectrum is shown as curve (iv) in Fig. l(a). External compression with chirped mirrors provides 30 fs pulses. The average power is 480 mW, implying a pulse energy of 1.1 nJ. 100
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Harmonic generation microscopy of dental sections Lasing action in air induced by ultrafast laser filamentation A 420 MHz Cr:forsterite femtosecond ring laser and its use for continuum generation in the 1-2 micron range Many particle theory for optical gain in quantum cascade lasers Microdisks with quantum dot active regions lasing near 1300 nm at room-temperature
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