3.6μm和1.55μm大气透射率的对比研究

R. Mahon, H. R. Burris, M. Ferraro, C. Moore, W. Rabinovich, M. Suite, W. Bewley, C. Canedy, D. Larrabee, J. R. Meyer, I. Vurgaftman
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引用次数: 4

摘要

在自由空间光链路中使用1.55μm激光器已经得到了广泛的应用。虽然人们期望在3.6μm下工作有优势,即通过水蒸气的更高透射率和更少的闪烁,但中红外波长的激光器和探测器的可用性并不像在1.55μm的电信选择中那样成熟。然而,有一些潜在的方案可以利用频率转换来探测中红外的大气,而在近红外中进行探测。在切萨皮克湾长达16公里的单向通道上进行了一系列实验,直接比较了两种波长下大气施加的强度差异和功率谱。采用带间级联激光器,工作波长为3.6μm,输出功率为100mW。1.55μm系统采用标准的电信部件。数据以4kHz的频率同时从两个系统中记录下来,并使用16位卡进行数字化。为了测量大气结构常数Cn2,望远镜测量了1.55毫米光束的到达角方差。此外,能见度监测器和气象站通常在线路的两端运作。
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A comparative study of 3.6μm and 1.55μm atmospheric transmission
The use of 1.55μm lasers for free space optical links has become well established. While one expects there to be advantages to operating at 3.6μm, namely higher transmission through water vapor and reduced scintillation, the availability of both lasers and detectors at the mid IR wavelength is not as mature as those available at the telecomm choice of 1.55μm. However, there are potential schemes for using frequency conversion to probe the atmosphere in the mid-ir but to detect back in the near-ir. A sequence of experiments has been conducted, over a 16km one-way link across the Chesapeake Bay, to directly compare the intensity variances and the power spectrum imposed by the atmosphere at the two wavelengths. An interband cascade laser was used which operated at a wavelength of 3.6μm and had an output power of 100mW. The 1.55μm system used standard telecomm parts. Data were recorded simultaneously from both systems at 4kHz and were digitized using a 16-bit card. A telescope measured the angle-of-arrival variance of the 1.55mm beam in order to give a measure of the atmospheric structure constant Cn2. In addition a visibility monitor and weather station were usually operational at each end of the link.
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