Z-scan measurements of nonlinear refraction in Yb3+: KY(WO4)2

V. Mikhailov, P. V. Prokoshin, K. Yumashev, N. N. Posnov, V. Kozich
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Abstract

Recently, laser performance of new Yb3+: KY(WO4)2 crystal (Yb3+:KYW) has been obtained at 1025 nm [1]. The Yb3+:KYW crystal is promising for the microchip and passive mode-locked lasers tuning in the range of 1020-1060 nm. It is known that Kerr-lens mode-locking technique based on the nonlinear refractive index n2 of the laser medium itself is a manner for femtosecond laser pulse generation. Such a regime on Yb3+:KYW crystal is in progress. The efficiency of Kerr-lens mode-locking depends on the n2 magnitude, and it is very important to know the n2 of laser medium for the development of Kerr-lens mode-locking. In this paper, the nonlinear refractive index of the Yb3+:KYW crystal has been measured using the Z-scan technique with a picosecond laser pulses Using a single laser beam in a tight focus geometry one measures the transmittance of a nonlinear medium through a finite aperture in the far field as a function of the sample position z measured with respect to the focal plane. The 15-ps laser pulses having an energy of 0.45 mJ are focused into the sample to the beam waist of 80 µm Figure shows a Z-scan of a 1.5 mm thick Yb3+:KY(WO4)2 crystal which has no absorption at 1.08 µm. The curve displays positive induced changes in the refractive index, and, as consequence, positive sign of n2. The index change is calculated from the phase distortion ϕ(z,r) in the sample, which is found from fitting experimental and model curves using “Gaussian decomposition” method.
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Yb3+: KY(WO4)2中非线性折射的z扫描测量
最近,新的Yb3+:KY (WO4)2晶体(Yb3+:KYW)在1025 nm处获得了激光性能[1]。Yb3+:KYW晶体在1020- 1060nm范围内的微芯片和无源锁模激光器调谐中具有广阔的应用前景。基于激光介质本身的非线性折射率n2的克尔透镜锁模技术是飞秒激光脉冲产生的一种方式。在Yb3+:KYW晶体上,这一过程正在进行中。克尔透镜锁模的效率取决于激光介质的n2大小,了解激光介质的n2大小对于克尔透镜锁模的发展是非常重要的。本文采用皮秒激光脉冲的z扫描技术测量了Yb3+:KYW晶体的非线性折射率。采用紧聚焦几何形状的单束激光,测量了非线性介质在远场通过有限孔径的透射率,作为所测样品位置z相对于焦平面的函数。将能量为0.45 mJ的15-ps激光脉冲聚焦到样品束腰80µm处,如图所示为1.08µm处无吸收的1.5 mm厚Yb3+:KY(WO4)2晶体的z轴扫描图。曲线显示正诱导的折射率变化,因此,n2的正号。指数的变化是从样品中的相位畸变φ (z,r)计算出来的,这是通过使用“高斯分解”方法拟合实验曲线和模型曲线得到的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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