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100 THz bandwidth of optical parametric amplification in the near-IR using bismuth triborate crystals pumped at 800 nm

机译:近红外的光学参数放大的100 THz带宽使用铋与800nm泵送的铋rucistate晶体

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The concept of ultrabroadband (more than one octave) coherent amplification relies on optical parametric amplification (OPA) at achromatic phase-matching condition defined by zero group velocity mismatch (GVM) between the idler and signal pulses. In the case of a collinear type-I interaction, this condition is always fulfilled near the degeneracy wavelengths (λ{sub}S≈λ{sub}I), but the bandwidth can be further enhanced if the group velocity dispersion (GVD) of the signal and idler waves also vanishes. In this case the gain bandwidth can reach an octave value and it is determined by the fourth derivative of the wave vector mismatch with respect to frequency, at the phase matching point. Unfortunately, in birefringent nonlinear crystals like BBO, most often used for ultrabroadband OPA [1], the second condition is simultaneously fulfilled at pump wavelengths λ{sub}p far from the 800 nm spectral range, in which high-power femtosecond Ti:sapphire laser systems operate with high stability at kHz repetition rates.
机译:超载带(多个八度音阶)相干放大的概念依赖于在惰轮和信号脉冲之间由零组速度失配(GVM)定义的消色差相位匹配条件的光学参数(OPA)。在共线型-I交互的情况下,在退化波长附近(λ{sub}s≈λ{sub} i)附近始终满足该条件,但是如果群体速度色散(GVD),则可以进一步增强带宽。信号和惰轮波也消失了。在这种情况下,增益带宽可以达到倍增值值,并且在相位匹配点处由波矢量错配的第四导数决定。不幸的是,在双折射非线性像BBO晶体,最常用于超宽带OPA [1],第二条件被同时在泵浦波长λ{子} p从800纳米的光谱范围内,实现远其中高功率飞秒钛:蓝宝石激光系统在KHz重复率下具有高稳定性。

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