首页> 外文会议>Optical Trapping and Optical Micromanipulation IV; Proceedings of SPIE-The International Society for Optical Engineering; vol.6644 >Improving optical trapping in the axial direction and a continuous change of the optimal trapping depth
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Improving optical trapping in the axial direction and a continuous change of the optimal trapping depth

机译:改善轴向的光陷波并不断改变最佳陷波深度

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Oil immersion objectives have higher numerical aperture than water immersion objectives thus providing higher optical resolution. This is important for confocal microscopy as well as for the strength of an optical trap created by such an objective, because the efficiency of an optical trap is limited by its axial strength. However, light focused by oil immersion objectives suffer from spherical aberrations caused e.g. by a mismatch between the refractive index of the immersion and sample media. Such aberrations widen the intensity profile in the focal region thus restricting the axial resolution of the objective and decreasing the axial optical trapping strength. Objectives are typically designed such that the spherical aberrations are minimized for visible wavelengths and a few microns away from the surface. However, often optical traps are based on infrared lasers or are used further away from the surface thus introducing considerable spherical aberrations. We have shown that a tuning of the immersion refractive index can minimize the total spherical aberrations at any desired depth, thus maximizing the trapping efficiency and giving rise to optical trapping strengths twice as large as previously reported. Changing the immersion media, however, is a discrete way of tuning the optimal trapping depth: An increment (decrement) of 0.01 in the refractive index of the immersion media gives rise to an increase (decrease) of approx = 4μm and approx =10μm of the most efficient trapping depth for infinity-tube length and finite-tube length objectives, respectively. Here, we show that combining a change of immersion media with changing tube length provides a continuous way of changing the optimal trapping depth. Also, we show how trapping conditions change with polarization.
机译:油浸物镜比水浸物镜具有更高的数值孔径,从而提供更高的光学分辨率。这对于共聚焦显微镜以及由该物镜产生的光阱的强度很重要,因为光阱的效率受到其轴向强度的限制。然而,由油浸物镜聚焦的光遭受例如引起的球差。由于浸没和样品介质的折射率不匹配。这样的像差加宽了焦点区域中的强度分布,从而限制了物镜的轴向分辨率并降低了轴向光学捕获强度。通常设计物镜时,应使可见光波长的球差最小,并且离表面几微米。但是,光阱通常基于红外激光或在远离表面的地方使用,因此会引入相当大的球差。我们已经表明,调整浸没折射率可以使任何所需深度的总球差最小化,从而使捕获效率最大化,并产生两倍于先前报道的光学捕获强度。但是,更改浸入介质是调整最佳捕获深度的一种离散方法:浸入介质的折射率增加(减少)0.01会导致增加(减少)大约=4μm和大约=10μm。分别是无限管长度和有限管长度物镜的最有效陷获深度。在这里,我们表明,将浸没介质的变化与管长的变化结合在一起,可以提供一种连续的方式来改变最佳捕集深度。此外,我们展示了捕获条件如何随极化变化。

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