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基于波长调制和最小立方算法的增强暗场照明的荧光纳米粒子的增强 3D 超分辨

Augmented 3D super-resolution of fluorescence-free nanoparticles using enhanced dark-field illumination based on wavelength-modulation and a least-cubic algorithm.

机构信息

Department of Chemistry, Graduate School, Kyung Hee University, Yongin-si, Gyeonggi-do 17104, Republic of Korea.

Department of Applied Mathematics, Kyung Hee University, Yongin-si, Gyeonggi-do 17104, Republic of Korea.

出版信息

Sci Rep. 2016 Sep 13;6:32863. doi: 10.1038/srep32863.

DOI:10.1038/srep32863
PMID:27619347
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5020655/
Abstract

Augmented three-dimensional (3D) subdiffraction-limited resolution of fluorescence-free single-nanoparticles was achieved with wavelength-dependent enhanced dark-field (EDF) illumination and a least-cubic algorithm. Various plasmonic nanoparticles on a glass slide (i.e., gold nanoparticles, GNPs; silver nanoparticles, SNPs; and gold nanorods, GNRs) were imaged and sliced in the z-direction to a thickness of 10 nm. Single-particle images were then compared with simulation data. The 3D coordinates of individual GNP, SNP, and GNR nanoparticles (x, y, z) were resolved by fitting the data with 3D point spread functions using a least-cubic algorithm and collation. Final, 3D super-resolution microscopy (SRM) images were obtained by resolving 3D coordinates and their Cramér-Rao lower bound-based localization precisions in an image space (530 nm × 530 nm × 300 nm) with a specific voxel size (2.5 nm × 2.5 nm × 5 nm). Compared with the commonly used least-square method, the least-cubic method was more useful for finding the center in asymmetric cases (i.e., nanorods) with high precision and accuracy. This novel 3D fluorescence-free SRM technique was successfully applied to resolve the positions of various nanoparticles on glass and gold nanospots (in vitro) as well as in a living single cell (in vivo) with subdiffraction limited resolution in 3D.

摘要

利用波长相关的增强暗场(EDF)照明和最小立方算法,实现了无荧光单纳米粒子的增强三维(3D)亚衍射极限分辨率。在玻璃载玻片上对各种等离子体纳米粒子(即金纳米粒子、GNPs;银纳米粒子、SNPs;和金纳米棒、GNRs)进行成像,并在 z 方向上切割到 10nm 的厚度。然后将单粒子图像与模拟数据进行比较。通过使用最小立方算法和整理拟合数据的 3D 点扩展函数,分别解析单个 GNP、SNP 和 GNR 纳米粒子的 3D 坐标(x、y、z)。最后,通过在图像空间(530nm×530nm×300nm)中解析 3D 坐标及其基于克拉美罗下界的定位精度,并在特定体素尺寸(2.5nm×2.5nm×5nm)下,获得 3D 超分辨率显微镜(SRM)图像。与常用的最小二乘法相比,最小立方法在具有高精度和准确性的不对称情况(即纳米棒)中更有助于找到中心。这种新型的无荧光 3D SRM 技术成功地应用于解析玻璃和金纳米点(体外)上各种纳米粒子的位置,以及在具有亚衍射极限分辨率的活单个细胞(体内)中的位置。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/2f4848af5dbe/srep32863-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/ef3e88b5dfd5/srep32863-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/272eb4a5ebad/srep32863-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/9c422aa3d8ce/srep32863-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/11947cdb712c/srep32863-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/d60ca4df564e/srep32863-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/c4026063c16a/srep32863-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/2f4848af5dbe/srep32863-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/ef3e88b5dfd5/srep32863-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/272eb4a5ebad/srep32863-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/9c422aa3d8ce/srep32863-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/11947cdb712c/srep32863-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/d60ca4df564e/srep32863-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/c4026063c16a/srep32863-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/256a/5020655/2f4848af5dbe/srep32863-f7.jpg

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