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Self-focusing in a BaTiO_3 crystal without external electric fields

机译:在BaTiO_3晶体中自动聚焦而无需外部电场

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Self-trapping in photorefractive materials is a well-known effect and was widely investigated during the past decade. Usually, the light induced Pockels effect in photorefractive crystals compensates the natural divergence of the beam, therefore, creating a beam with constant diameter, a spatial soliton. The Pockels effect is based on the redistribution of charges in the crystal and can be forced by an external electric field. Due to the crystallographic structure of their elementary cell (tetragonal phase for temperatures below the Curie temperature) some crystals as BaTiO_3 or SBN possess a preferential direction the so called c-axis. They are spontaneously poled but in a statistical manner. Applying an external electric field with temperatures higher than the Curie-temperature and then decreasing the temperature all elementary cells will be orientated in the same direction, the crystal will be poled. This poling remains even if the external field is switched off. This means that the crystal obtains a remanent internal electric polarization. The experiment shows that this internal polarization can be understood as an effective electric field and, therefore, the self-focusing of appropriate laser beams is possible. We show the self-focusing of beams of a HeNe-laser (λ = 633 nm, P = 0.1 μW, 2w_0 = 4 μm) in BaTiO_3 without external electric fields and discuss the effect in dependence on the polarization and the intensity of the light beam at the entrance surface of the crystal. The experimental results are compared with numerical solutions of the stationary paraxial normalized wave equation.
机译:在光折射材料中自陷是一种众所周知的效应,并且在过去的十年中进行了广泛的研究。通常,光折射晶体中的光诱导普克尔斯效应会补偿光束的自然发散,因此会产生具有恒定直径的光束,即空间孤子。普克尔斯效应是基于晶体中电荷的重新分布,并可能受到外部电场的强迫。由于其基本晶胞的晶体结构(温度低于居里温度时为四方晶),BaTiO_3或SBN等晶体具有优先的方向,即所谓的c轴。它们自发地极化,但以统计方式。施加温度高于居里温度的外部电场,然后降低温度,所有基本单元将沿相同方向取向,晶体将极化。即使关闭外部磁场,这种极化仍然存在。这意味着晶体获得剩余的内部极化。实验表明,这种内部偏振可以理解为有效电场,因此可以对合适的激光束进行自动聚焦。我们展示了在没有外部电场的情况下,HeNe激光束(λ= 633 nm,P = 0.1μW,2w_0 = 4μm)在没有外电场的情况下的自聚焦,并讨论了依赖于偏振和光强度的影响光束进入晶体的入射面。将实验结果与固定近轴归一化波动方程的数值解进行了比较。

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