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Two-color excitation fluorescence microscopy through highly scattering media

机译:通过高散射介质的双色激发荧光显微镜

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We study the performance of two-color excitation (2CE) fluorescence microscopy [Opt. Lett. 24, 1505 (1999)] in turbid media of different densities and anisotropy. Excitation is achieved with two confocal excitation beams of wavelengths λ_(1) and λ_(2), which are separated by an angular displacement θ, where λ_(1)≠λ_(2), 1/λ_(e)=1/λ_(1)+1/λ_(2), and λ_(e) is the single-photon excitation wavelength of the sample. 2CE fluorescence is generated only in regions of the sample where the two excitation beams overlap. The 2CE fluorescence intensity is proportional to the product of the two excitation intensities and could be detected with a large-area photodetector. The requirement of spatiotemporal simultaneity for the two excitation beams makes 2CE fluorescence imaging a promising tool for observing microscopic objects in a highly scattering medium. Optical scattering asymmetrically broadens the excitation point-spread function and toward the side of the focusing lens that leads to the contrast deterioration of the fluorescence image in single- or two-photon (λ_(1)=λ_(2)) excitation. Image degradation is caused by the decrease in the excitation energy density at the geometrical focus and by the increase in background fluorescence from the out-of-focus planes. In a beam configuration with θ≠0, 2CE fluorescence imaging is robust against the deleterious effects of scattering on the excitation-beam distribution. Scattering only decreasea the available energy density at the geometrical focus and does not increase the background noise. For both isotropic and anisotropic scattering media the performance of 2CE imaging is studied with a Monte Carlo simulation for θ=0, π/2, and π, and at different h/d_(s) values where h is the scattering depth and d_(s) is the mean-free path of the scattering medium.
机译:我们研究了双色激发(2CE)荧光显微镜的性能[Opt。来吧24,1505(1999)]在不同密度和各向异性的混浊介质中。激发是通过两个共焦激发光束实现的,它们的波长分别为λ_(1)和λ_(2),它们被角位移θ分开,其中λ_(1)≠λ_(2),1 /λ_(e)= 1 /λ_ (1)+ 1 /λ_(2),λ_(e)是样本的单光子激发波长。 2CE荧光仅在两个激发光束重叠的样品区域中产生。 2CE荧光强度与两个激发强度的乘积成正比,可以用大面积光电探测器检测到。两个激发光束的时空同步性要求使2CE荧光成像成为观察高散射介质中的微观物体的有前途的工具。光学散射不对称地扩展了激发点扩展功能,并朝着聚焦透镜的一侧扩散,这导致了单光子或双光子(λ_(1)=λ_(2))激发中荧光图像的对比度下降。图像质量下降是由于几何焦点处激发能量密度的降低以及来自离焦平面的背景荧光的增加所致。在具有θ≠0的光束配置中,2CE荧光成像可抵抗散射对激发光束分布的有害影响。散射只会降低几何焦点处的可用能量密度,而不会增加背景噪声。对于各向同性和各向异性散射介质,通过蒙特卡罗模拟对θ= 0,π/ 2和π以及在不同的h / d_(s)值下研究2CE成像的性能,其中h是散射深度和d_( s)是散射介质的平均自由程。

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