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Broadband mid-IR subharmonic OPOs for molecular spectroscopy

机译:宽带中红外亚谐波OPO用于分子光谱

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We generate broadband mid-infrared frequency combs via degenerate optical parametric oscillation in a subharmonic OPO. This technique efficiently transfers the desirable properties of shorter wavelength mode-locked sources to the mid-IR. Our OPO resonator is a 3m or 4m ring cavity composed of one pair of concave mirrors with R=50mm and four flat mirrors, all but one of which are gold coated with > 99% reflection. A single dielectric mirror is used to introduce the pump (2.05 micron from IMRA America, 75 MHz, 80 fs, 600mW or 1.55 micron from Menlo Systems C-fiber, 100 MHz, 70 fs, 350 mW or 1.56 micron from Toptica Photonics FemtoFiber Pro, 80 MHz, 85 fs, 380 mW). The dielectric mirror is transmissive for the pump and reflective in a 2.5- 4 micron or 3- 6 micron (for 2 micron pump) range. Broadband parametric gain around the 3.1-micron subharmonic is provided by short (0.2-0.5mm) periodically poled lithium niobate (MgO:PPLN) at Brewster angle. Crystals were cut from Crystal Technology Inc. material having QPM period of 34.8 microns for type 0 (e=e+e) phase matching at t=32 deg. C. With the 2-micron pump, orientation patterned gallium arsenide from BAE systems is used as the non-linear material In both systems, the enormous acceptance bandwidth at degeneracy, typical for OPOs with type 0 (or type I) phase-matching, gives broad bandwidth and makes temperature tuning insignificant. Broadband oscillation is achieved when signal/idler are brought into degenerate resonance by fine-tuning the cavity length with a mirror on a piezo stage. Using an 8% reflective pellicle, we outcouple a frequency comb of more than 1000nm bandwidth, centered around 3.1 microns from the Er/PPLN system. A lmm or 2.5mm thick ZnSe plate at Brewster angle provides 2nd-order group velocity dispersion compensation, improving the OPO bandwidth. The OPO threshold was measured to be < 30mW. When locked, the OPO outputs 60 mW of average power centered at 3.1 microns. With the Tm/OP-GaAs system we achieve octave-spanning output from 3- 6 micron using a mix of YAG and CaF for dispersion compensation and output powers over 30 mW.
机译:我们通过次谐波OPO中的简并光学参量振荡生成宽带中红外频率梳。该技术有效地将较短波长锁模光源的理想特性传递给中红外。我们的OPO谐振器是一个3m或4m环形腔,由一对R = 50mm的凹面镜和四个平面镜组成,除一个平面镜外,其他所有镜面均镀金,反射率大于99%。使用单个介电镜引入泵(来自IMRA America的2.05微米,来自Menlo Systems C-光纤的75 MHz,80 fs,600mW或1.55微米,来自Toptica Photonics FemtoFiber Pro的100 MHz,70 fs,350 mW或1.56微米) ,80 MHz,85 fs,380 mW)。介电镜对于泵是透射的,并且在2.5-4微米或3-6微米(对于2微米泵)范围内反射。 3.1微米亚谐波周围的宽带参数增益由布鲁斯特角上的短(0.2-0.5mm)周期性极化的铌酸锂(MgO:PPLN)提供。从具有34.8微米QPM周期的Crystal Technology Inc.材料中切出晶体,以在t = 32度时进行0型(e = e + e)相匹配。 C.使用2微米泵,将BAE系统中的定向图案化砷化镓用作非线性材料。在这两个系统中,简并性具有巨大的接受带宽,这对于具有0型(或I型)相位匹配的OPO来说是典型的,提供宽带宽,并且温度调节微不足道。通过使用压电镜上的反射镜微调腔体长度,使信号/闲置信号发生简并谐振,可以实现宽带振荡。使用8%的反射膜,我们将Er / PPLN系统的中心频率约为3.1微米的带宽梳齿耦合到1000nm以上。布鲁斯特角处的1mm或2.5mm厚的ZnSe板可提供二阶群速度色散补偿,从而改善了OPO带宽。 OPO阈值测得小于30mW。锁定时,OPO输出以3.1微米为中心的60 mW平均功率。借助Tm / OP-GaAs系统,我们使用YAG和CaF的混合物实现了3至6微米的倍频程输出,以进行色散补偿,并且输出功率超过30 mW。

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