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Lasing characteristics of optically pumped edge-emitting organic semiconductor laser

机译:光泵浦边缘发射有机半导体激光器的激光特性

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Last year, we succeeded in reproducibly producing optically pumped edge-emitting organic semiconductor lasers using a low-temperature cleaving technique. Since the organic layer was generally soft and weak, its edge was damaged by the conventional cleaving at room temperature. This damage reduces the reflectance at the mirror edge and increases the threshold excitation energy. Stiffening the organic layer in liquid nitrogen enabled us to produce high-quality resonators with sufficient reproducibility. Slab waveguide devices consisting of Alq_3:DCM film (5% DCM) were vacuum-deposited onto a polished GaAs (100) substrate coated with an l-μm-thick layer of RF (radio-frequency) sputtered SiO_2-^sThe cleaved samples were optically pumped by a N_2 gas laser (wavelength: 337 nm) resulting in a pulse width of 600 ps at repetition rate of 20 Hz. The laser oscillation was checked by measuring the full width at half maximum of the output spectrum and its polarization characteristics. The threshold density was typically 3 μJ/cm~2 in a sample with a 5-mm-long resonator. We investigated the relationship between the resonator loss and the threshold density by varying the resonator length. The internal loss α and the gain coefficient β were found to be about 10.5 cm~(-1) and 3.2 μJ~(-1)cm, respectively. The threshold density was calculated as a function of the thickness of the emitting layer and compared with experimental values. We found that the optimum thickness is approximately 150 nm. Moreover, the reflectance at the mirror edge was increased by attaching a metal (aluminum) reflector to one side, resulting in a reduction in the threshold.
机译:去年,我们成功地使用低温切割技术可重复地生产光学泵浦边缘发射有机半导体激光器。由于有机层通常柔软且弱,因此其边缘在室温下通过常规切割损坏。这种损坏降低了镜面边缘处的反射率,并增加了阈值激励能量。使液氮中的有机层加强使我们能够生产具有足够可重复性的高质量谐振器。将由Alq_3:DCM膜(5%DCM)组成的平板波导器件被真空沉积到涂覆有L-μm厚的RF(射频)溅射的SiO_2- ^ STHE切割样品的抛光GaAs(100)底板上通过N_2气体激光(波长:337nm)光学泵送,导致脉冲宽度为20Hz的重复率为600ps。通过测量输出频谱的半最大值及其偏振特性,通过测量全宽来检查激光振荡。阈值密度通常在具有5mm长的谐振器的样品中为3μJ/ cm〜2。我们通过改变谐振器长度来研究谐振器损耗与阈值密度之间的关系。内部损耗α和增益系数β分别为约10.5cm〜(-1)和3.2μj〜(-1)厘米。计算阈值密度作为发光层的厚度并与实验值进行比较。我们发现最佳厚度约为150nm。此外,通过将金属(铝)反射器连接到一侧,增加了镜面边缘的反射率,导致阈值的降低。

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