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Fe∶ZnMnSe laser active material properties at room and cryogenic temperature

机译:Fe:znmnse激光有源材料在室内和低温温度

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Fe∶Zn(1-x)Mn(x)Se solid solution spectroscopic and laser properties were investigated in the temperature range 80-290 K. Two novel samples with different zinc - manganese (Zn-Mn) ratio described by the Mn content x (0.1 or 0.2) were used and the results were compared to the known Fe∶ZnSe crystal. The samples had a broad absorption spectra with the maximum around 3 μm and therefore an Er∶YAG laser (2.94 μm, 10 mJ, 120 ns) was used as a pump radiation source. The Fe:ZnMnSe fluorescence spectra are generally broad in the range 3.5 - 5.5 μm. In the case of Fe∶ZnMnSe x = 0.1, the fluorescence spectrum at 290 K is ranging from 3.5 to 5.5 μm. Lowering the temperature down to 80 K lead to the spectral narrowing mainly in the mid-IR part, but the fluorescence is still up to 5 μm at 80 K. In the case of Fe∶ZnMnSe x = 0.2 the fluorescence is shifted towards mid-IR up to 5.2 μm even at 80 K. The fluorescence lifetime decreases from tens of us at 80 K down to 1 us at 240 K. The laser oscillations were successfully achieved with both novel Fe∶ZnMnSe crystals in the temperature range 80- 290 K. In the case of x = 0.1, the central wavelength was ~4.2 μm at 80 K and the temperature increase up to 290 K led to almost linear increase of the wavelength up to ~4.75 μm. The tendency was similar in the case of Fe∶ZnMnSe x = 0.2: the output wavelength increased from ~4.3 μm up to ~4.8 μm with the temperature increase from 80 to 290 K. The laser spectral linewidth was about 300 ran. In comparison with the Fe∶ZnSe crystal, the laser output wavelength shift toward mid-IR region without any spectrally tunable element in the laser cavity can be clearly observed.
机译:的温度范围内Fe:Zn(1-X)的Mn(x)的硒固溶光谱和激光性能进行了研究80-290具有不同锌K.两种新的样本 - 锰(锌 - 锰)的比例通过使Mn含量x描述(0.1或0.2)中使用,并将结果与​​已知Fe:ZnSe晶体。样品具有与约3微米的最大,因此被用作泵浦辐射源的Er:YAG激光(2.94微米,10毫焦耳,120纳秒)宽的吸收光谱。中的Fe:ZnMnSe荧光光谱通常在广泛的范围内3.5 - 5.5微米。在Fe:ZnMnSe X = 0.1的情况下,在290 K的荧光光谱范围为3.5至5.5微米。降低温度下降到80K时导致的频谱收缩主要在中红外部分,但荧光仍可达5微米,在80 K.在X = 0.2的荧光朝中期移位Fe:ZnMnSe的情况下IR高达5.2微米,即使在80 K.荧光寿命从几十我们的在80K时下降到1我们在240 K的激光振荡用既新颖Fe:ZnMnSe晶体的温度范围内80〜290ķ成功地实现减小。在x = 0.1的情况下,中心波长为〜4.2微米,在80 K和温度增大到290ķ导致波长上的几乎线性增加至〜4.75微米。的趋势是在Fe:ZnMnSe为x = 0.2的情况下相似的:输出波长从4.3〜向上微米增加至〜4.8微米与温度增加80至290 K.激光光谱线宽约为300 RAN。与Fe:ZnSe晶体比较,激光输出波长偏移朝向中红外区而不在激光腔中的任何光谱可调谐元件可以清楚地观察。

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