基于倏逝波照明的空间频移超分辨成像研究

None Ling Jin-Zhong, None Guo Jin-Kun, None Wang Yu-cheng, None Liu Xin, None Wang Xiao-rui
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Another deficiency of this scheme is the difference of imaging resolution in different directions, as only in the direction along the wave vector of illumination evanescent wave, the image has the highest resolution; while in the direction perpendicular to it, the image has the lowest resolution, as same as that obtained by far-field illumination.<br/>In order to solve the above thorny questions, a new model for evanescent wave generation has been proposed, which could generate omnidirectional evanescent wave with arbitrary wavelength based the phase modulation of nano-structure, and solve the both problem in imaging system at the same time. To verify the possibility of our scheme, we set up a complete simulation model for spatial frequency shift imaging scheme, which includes three parts:the generation of evanescent wave and its interaction with the nano-structures at imaging target, with could be simulated with FDTD algorithm; the propagation of light field from near-field to far-field, from the sample surface to the focal plane of objective lens, which could be calculated with angular spectrum theory; the propagation of light field from the focal place to the image plane, which could be calculated with Chirp-Z transform.<br/>With this complete simulation model, we compared the resolution of microscopy illuminated by evanescent wave and propagating wave, firstly. 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引用次数: 0

摘要

尽管荧光显微镜(如STED、STORM和PALM)在生物医学领域取得了成功,实现了纳米级成像分辨率,促进了生物医学的巨大发展,但非荧光样品的超分辨率成像方法仍然稀缺,分辨率与纳米级仍有很大差距。在现有的方法中,结构照明显微镜、PSF工程、超振荡透镜和微球辅助纳米显微镜技术较为成熟,应用较为广泛。然而,受理论本身或工程实践的限制,这些方法的分辨率很难突破50 nm,这限制了它们在许多领域的应用。<br/>在合成孔径技术的启发下,研究人员通过移动和组合成像目标的空间频谱,提出了空间频移超分辨率显微镜。它的分辨率极限可以不断突破,是一种很有前途的超分辨率成像方案。目前,由于光学材料折射率的限制,在棱镜表面经全内反射产生的照明倏逝波波长难以缩短,这决定了该空间频移超分辨成像系统的最高分辨率。该方案的另一个不足是成像分辨率在不同方向上存在差异,只有在照明倏逝波的波矢量方向上,图像的分辨率才最高;为解决上述棘手的问题,本文提出了一种新的倏逝波产生模型,该模型可以基于纳米结构的相位调制产生任意波长的全向倏逝波,同时解决了成像系统中的这两个问题。为了验证该方案的可行性,我们建立了一个完整的空间频移成像方案的仿真模型,该模型包括三个部分:倏逝波的产生及其与成像目标纳米结构的相互作用,可以用FDTD算法进行模拟;光场从近场到远场,从样品表面到物镜焦平面的传播,可以用角谱理论计算;用Chirp-Z变换可以计算出光场从焦点到像面的传播。<br/>在这个完整的仿真模型下,我们首先比较了倏逝波和传播波照射下显微镜的分辨率。结果验证了倏逝波照明的超分辨成像能力,同时也证明了棱镜折射率的影响,折射率越高,倏逝波波长越短,空间频移成像系统的分辨率越高。其次,我们演示了三棒成像目标旋转不同方向时在一系列方向上的分辨率差异。结果表明,成像分辨率最高的方向为照明倏逝波矢量方向,成像分辨率最低的方向为垂直于照明倏逝波矢量方向。最后,对纳米结构产生的倏逝波进行了模拟,验证了其波长特性和矢量方向特性。当应用于近场照明超分辨成像时,全向倏逝波解决了棱镜表面全内反射模型存在的这两个问题。因此,我们方案的优点是成像分辨率更高,成像速度更快,不需要多方向多次成像,无需图像后处理。我们的研究为空间频移超分辨率成像开辟了一个新的视角,为其应用奠定了理论基础。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Research on spatial frequency shift super-resolution imaging based on evanescent wave illumination
In spite of the success of fluorescence microscopes (such as STED, STORM and PALM) in biomedical field, which have realized nanometer scale imaging resolution and promoted the great development of bio-medicine, the super-resolution imaging method for non-fluorescent sample is still scarce, and the resolution still has a big gap to nanometer scale. Among existing methods, structured illumination microscopy, PSF engineering, super-oscillatory lens and microsphere assisted nanoscopy are more mature and widely applied. However, limited by the theory itself or engineering practice, the resolution of these approaches is hard to break through 50 nm, which restricts their application in many fields.
Enlightened by synthetic aperture technique, researchers proposed spatial frequency shift super-resolution microscopy through shifting and combining the spatial frequency spectrum of imaging target, which is a promising super-resolution imaging scheme as its resolution limit could be broken through continually. Currently, due to the restriction of the refractive index of optical materials, the wavelength of illumination evanescent wave is hard to be shorten when generated at prism surface via total internal reflection, which determines the highest resolution of this spatial frequency shift super-resolution imaging system. Another deficiency of this scheme is the difference of imaging resolution in different directions, as only in the direction along the wave vector of illumination evanescent wave, the image has the highest resolution; while in the direction perpendicular to it, the image has the lowest resolution, as same as that obtained by far-field illumination.
In order to solve the above thorny questions, a new model for evanescent wave generation has been proposed, which could generate omnidirectional evanescent wave with arbitrary wavelength based the phase modulation of nano-structure, and solve the both problem in imaging system at the same time. To verify the possibility of our scheme, we set up a complete simulation model for spatial frequency shift imaging scheme, which includes three parts:the generation of evanescent wave and its interaction with the nano-structures at imaging target, with could be simulated with FDTD algorithm; the propagation of light field from near-field to far-field, from the sample surface to the focal plane of objective lens, which could be calculated with angular spectrum theory; the propagation of light field from the focal place to the image plane, which could be calculated with Chirp-Z transform.
With this complete simulation model, we compared the resolution of microscopy illuminated by evanescent wave and propagating wave, firstly. The results verified the super-resolution imaging ability of evanescent wave illumination, and also demonstrated the influence of refractive index of prism, as higher refractive index makes shorter wavelength of evanescent wave and higher resolution of spatial frequency shift imaging system. Secondly, we demonstrated the resolution difference at a series directions with a three-bar imaging target rotated to different directions. The result shows that the highest imaging resolution occurs at the direction of illumination evanescent wave vector, and the lowest resolution appears at the direction perpendicular to the wave vector. At last, we simulated the evanescent wave generated by nano-strcuture and demonstrated its properties of wavelength and vector direction. When applied to near-field illumination super-resolution imaging, the omnidirectional evanescent wave solved the both problems existing in the model of total internal reflection at prism surface.
Therefore, the advantages of our scheme are higher imaging resolution and faster imaging speed, no need for multi-direction and multiple imaging, and also image post-processing. Our research opened up a new perspective of spatial frequency shift super-resolution imaging, and established a theoretical foundation for its application.
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