用于多波长双光子显微镜的PCF红外连续体

C. de Mauro, D. Alfieri, M. Arrigoni, D. Armstrong, F. Pavone
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引用次数: 0

摘要

由于飞秒脉冲耦合到光子晶体光纤(PCFs)中所产生的非线性,可以从单波长激光开始产生连续光谱。多光子显微镜[1]、荧光寿命成像[2]、受激发射耗尽显微镜[3]、光学相干断层成像[4]等已经在此激励源上实现,涵盖了目前最先进的生物成像技术。通常利用聚苯乙烯的异常色散和高非线性特性来产生更大的光谱展宽。我们选择在正常色散区域泵送具有选定色散曲线的PCF。这种方法的效果是:减少了非线性,输出频谱平坦,降低了不同频谱带产生的[5]的幅度噪声。我们主要从两方面来描述系统的成像性能。首先利用亚分辨率荧光珠测量点扩展函数(PSF),实现了整个光谱的亚微米径向分辨率和微米光学切片。最重要的是,我们将从780nm附近的连续体中选择30nm宽波段获得的图像与使用单一波长785nm光源获得的图像进行了比较(见图1):信噪比(SNR)和图像质量相当,从而证明了我们方法的有效性。然后,光纤输出端的光谱可以任意成形,以在700nm至1000nm范围内选择所需的激发波长,其中最常见的荧光团的两个光子横截面达到峰值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
PCF infrared continuum for multiwavelength two photon microscopy
Thanks to the non linearity arising when femtosecond pulses are coupled into Photonic Crystal Fibers (PCFs), continuum spectra can be generated starting from single wavelength lasers. Multiphoton microscopy [1], fluorescence lifetime imaging [2], stimulated emission depletion microscopy [3], and optical coherence tomography [4] have been previously realized using such kind of excitation source, covering most of the state-of-the-art biological imaging techniques. Usually the properties of PCFs in terms of anomalous dispersion and high non linearity are exploited to produce the greater spectral broadening. We choose instead to pump a PCF with a selected dispersion profile in the normal dispersion region. This approach results in effects: reduction of non linearity, flat spectrum at the output and reduced amplitude noise in the different spectral bands generated [5]. We characterize the imaging performances of the system mainly in two ways. First of all by measuring the Point Spread Function (PSF) using sub-resolution fluorescent beads: sub micron radial resolution and micron optical sectioning is achieved in the whole spectrum. Most important, we compared the images obtained with a 30nm wide band selected from the continuum around 780nm with the ones using a single wavelength 785nm source (see Fig.1): Signal to Noise Ratio (SNR) and image quality are comparable, thus demonstrating the validity of our approach. The spectrum at the output of the fiber can then be arbitrarily shaped to select the desired excitation wavelength in the range from 700nm to 1000nm, where the two photon cross sections of the most common fluorophores are peaked.
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