1,030 research outputs found
Fast and robust single particle reconstruction in 3D fluorescence microscopy
Single particle reconstruction has recently emerged in 3D fluorescence
microscopy as a powerful technique to improve the axial resolution and the
degree of fluorescent labeling. It is based on the reconstruction of an average
volume of a biological particle from the acquisition multiple views with
unknown poses. Current methods are limited either by template bias, restriction
to 2D data, high computational cost or a lack of robustness to low fluorescent
labeling. In this work, we propose a single particle reconstruction method
dedicated to convolutional models in 3D fluorescence microscopy that overcome
these issues. We address the joint reconstruction and estimation of the poses
of the particles, which translates into a challenging non-convex optimization
problem. Our approach is based on a multilevel reformulation of this problem,
and the development of efficient optimization techniques at each level. We
demonstrate on synthetic data that our method outperforms the standard
approaches in terms of resolution and reconstruction error, while achieving a
low computational cost. We also perform successful reconstruction on real
datasets of centrioles to show the potential of our method in concrete
applications
์ก์์ ์กด์ฌํ๋ ๊ฐ๋ณ ๋๋ ธ์ ์์ ๋ํ 3์ฐจ์ ์์๊ตฌ์กฐ ๋ถ์ ๋ฐฉ๋ฒ๋ก
ํ์๋
ผ๋ฌธ(๋ฐ์ฌ) -- ์์ธ๋ํ๊ต๋ํ์ : ๊ณต๊ณผ๋ํ ํํ์๋ฌผ๊ณตํ๋ถ, 2023. 2. ๋ฐ์ ์.Precise three-dimensional (3D) atomic structure determination of individual nanocrystals is a prerequisite for understanding and predicting their physical properties, because the 3D atomic arrangements of materials determine the free energy landscape. We developed a Brownian one-particle reconstruction based on imaging of ensembles of colloidal nanocrystals using graphene liquid cell electron microscopy.
Nanocrystals from the same synthesis batch display what are often presumed to be small but possibly important differences in size, lattice distortions, and defects, which can only be understood by structural characterization with high spatial 3D resolution. The structures of individual colloidal platinum nanocrystals are solved by developing atomic-resolution 3D liquid-cell electron microscopy to reveal critical intrinsic heterogeneity of ligand-protected platinum nanocrystals in solution, including structural degeneracies, lattice parameter deviations, internal defects, and strain. These differences in structure lead to substantial contributions to free energies, consequential enough that they must be considered in any discussion of fundamental nanocrystal properties or applications.
We introduce computational methods required for successful atomic-resolution 3D reconstruction: (i) tracking of the individual particles throughout the time series, (ii) subtraction of the interfering background of the graphene liquid cell, (iii) identification and rejection of low-quality images, and (iv) tailored strategies for 2D/3D alignment and averaging that differ from those used in biological cryoโelectron microscopy.
Characterization of lattice symmetry is important because the symmetry is strongly correlated with physical properties of nanomaterials. We introduce direct and quantitative analysis of lattice symmetry by using 3D atomic coordinates obtained by liquid-phase TEM. We investigate symmetry of entire unit-cells composing individual platinum nanoparticles, revealing unique structural characteristics of sub-3 nm Pt nanoparticles.
We here introduce a 3D atomic structure determination method for multi-element nanoparticle systems. The method, which is based on low-pass filtration and initial 3D model generation customized for different types of multi-element systems, enables reconstruction of high-resolution 3D Coulomb density maps for ordered and disordered multi-element systems and classification of the heteroatom type. Using high-resolution image datasets obtained from TEM simulations of PbSe, CdSe, and FePt nanoparticles that are structurally relaxed with first-principles calculations in the graphene liquid cell, we show that the types and positions of the constituent atoms are precisely determined with root mean square displacement (RMSD) values less than 24 pm. Our study suggests that it is possible to investigate the 3D atomic structures of synthesized multi-element nanoparticles in liquid phase.์ฌ๋ฃ์ 3D ์์ ๋ฐฐ์ด์ด ์์ ์๋์ง ํ๊ฒฝ์ ๊ฒฐ์ ํ๋ค๋ ์ ์ ๊ณ ๋ คํ์ ๋, ๊ฐ๋ณ ๋๋
ธ๊ฒฐ์ ์ ์ ํํ 3์ฐจ์(3D) ์์ ๊ตฌ์กฐ ๋ถ์์ ๋ฌผ๋ฆฌ์ ํน์ฑ์ ์ดํดํ๊ณ ์์ธกํ๊ธฐ ์ํด ํ์ ๋ถ๊ฐ๊ฒฐํ๋ค. ๋ณธ ์ฐ๊ตฌ์๋ ๊ทธ๋ํ ์ก์ฒด ์ธํฌ ํฌ๊ณผ ์ ์ ํ๋ฏธ๊ฒฝ์ ์ฌ์ฉํ์ฌ ์ฝ๋ก์ด๋ ๋๋
ธ์
์์ ์์๋ธ ์ด๋ฏธ์ง์ ๊ธฐ๋ฐ์ผ๋ก ํ๋ "๋ธ๋ผ์ด ๋จ์ผ ์
์ ์ฌ๊ตฌ์ฑ"์ ๊ฐ๋ฐํ๋ค.
๋์ผํ ํฉ์ฑ ๋ฐฐ์น์ ๋๋
ธ์
์๋ ํฌ๊ธฐ, ๊ฒฉ์ ์๊ณก ๋ฐ ๊ฒฐํจ ๋ฑ์์ ์ข
์ข
์์ง๋ง ์ค์ํ ๊ฒ์ผ๋ก ์ถ์ ๋๋ ๊ฒ์ผ๋ก ๊ฐ์ฃผ๋๋ ๊ตฌ์กฐ์ ์ฐจ์ด์ ์ด ์์ผ๋ฉฐ, ์ด๋ 3D ๊ณ ํด์๋ ๊ตฌ์กฐ ๋ถ์์ ์ํด์๋ง ์ดํดํ ์ ์๋ค. ๊ตฌ์กฐ์ ํดํ, ๊ฒฉ์ ๋งค๊ฐ๋ณ์ ํธ์ฐจ, ๋ด๋ถ ๊ฒฐํจ ๋ฐ ๋ณํ์ ํฌํจํ ๊ฐ๋ณ ์ฝ๋ก์ด๋ ๋ฐฑ๊ธ ๋๋
ธ์
์์ ๊ตฌ์กฐ์ ํน์ฑ์ ์์ ๋ถํด๋ฅ 3D ์ก์ฒด ์ธํฌ ์ ์ ํ๋ฏธ๊ฒฝ์ ๊ฐ๋ฐํ์ฌ ํ์ด๋ผ ์ ์๋ค. ์ด๋ฌํ ๊ตฌ์กฐ์ ์ฐจ์ด๋ ์์ ์๋์ง์ ์๋นํ ๊ธฐ์ฌ๋ฅผ ํ๋ฏ๋ก ๊ฒฐ๊ณผ์ ์ผ๋ก ๊ธฐ๋ณธ์ ์ธ ๋๋
ธ์
์ ํน์ฑ ๋๋ ์์ฉ์ ๋ํ ๋
ผ์์์ ๊ณ ๋ ค๋์ด์ผ ํ๋ค.
๋ณธ ๋
ผ๋ฌธ์์๋ ์ฑ๊ณต์ ์ธ ์์ ํด์๋ 3D ์ฌ๊ตฌ์ฑ์ ํ์ํ ๊ณ์ฐ ๋ฐฉ๋ฒ๋ก ์ ์๊ฐํ๋ค. ๊ทธ ๋ฐฉ๋ฒ๋ก ์๋ ๋ค์๊ณผ ๊ฐ์ ์๊ณ ๋ฆฌ์ฆ์ด ํฌํจ๋๋ค. (1) ์๊ณ์ด ์ด๋ฏธ์ง์์ ๊ฐ๋ณ ๋๋
ธ์
์๋ฅผ ์ถ์ ํ๋ ์๊ณ ๋ฆฌ์ฆ, (2) ๊ทธ๋ํ ์ก์ฒด ์
์ ๋ฐฐ๊ฒฝ ๋
ธ์ด์ฆ๋ฅผ ์ ๊ฑฐํ๋ ์๊ณ ๋ฆฌ์ฆ, (3) ์ ํด์๋ ์ด๋ฏธ์ง๋ฅผ ๊ฒ์ถ ๋ฐ ์ ๊ฑฐํ๋ ์๊ณ ๋ฆฌ์ฆ, (4) ๊ทน์ ์จ ์ ์ํ๋ฏธ๊ฒฝ์ ์ด์ฉํ ๋ฐ์ด์ค ์
์์ ์ฌ๊ตฌ์ฑ์ ์ฐ์ด๋ ์๊ณ ๋ฆฌ์ฆ๊ณผ๋ ๋ค๋ฅธ ๋๋
ธ์
์๋ง์ ์ํด์ ๊ณ ์๋ 2์ฐจ์/3์ฐจ์ ์ ๋ ฌ ์๊ณ ๋ฆฌ์ฆ.
๊ฒฉ์ ๋์นญ์ฑ์ ๋๋
ธ ๋ฌผ์ง์ ๋ฌผ๋ฆฌ์ ํน์ฑ๊ณผ ๊ฐํ ์๊ด๊ด๊ณ๊ฐ ์๊ธฐ ๋๋ฌธ์, ๊ฒฉ์ ๋์นญ์ฑ ๋ถ์์ ์ค์ํ๋ค. ๋ณธ ๋
ผ๋ฌธ์์๋ ์ก์ ํฌ๊ณผ ์ ์ ํ๋ฏธ๊ฒฝ์ ํตํด์ ์ป์ 3์ฐจ์ ์์ ์ขํ๋ฅผ ์ด์ฉํ์ฌ ๊ฒฉ์ ๋์นญ์ ์ง์ ์ , ์ ๋์ ์ผ๋ก ๋ถ์ํ ์ ์๋ ๋ฐฉ๋ฒ๋ก ์ ์๊ฐํ๊ณ ์ ํ๋ค. ๊ฐ๋ณ ๋ฐฑ๊ธ ๋๋
ธ์
์๋ฅผ ๊ตฌ์ฑํ๋ ์ ์ฒด unit cell์ ๋์นญ์ฑ์ ์กฐ์ฌํจ์ผ๋ก์จ, 3 ๋๋
ธ๋ฏธํฐ ์ดํ์ ๋ฐฑ๊ธ ๋๋
ธ์
์๊ฐ ๊ฐ๋ ๋
ํนํ ๊ตฌ์กฐ์ ํน์ง์ ๋ฐํ๋ด์๋ค.
๋ณธ ๋
ผ๋ฌธ์์๋ ๋ค์์ ๋๋
ธ์
์ ์์คํ
์ ์ํ 3์ฐจ์ ์์ ๊ตฌ์กฐ ๋ถ์๋ฒ์ ์๊ฐํ๊ณ ์ ํ๋ค. ์ ์๋ low-pass filtering๊ณผ initial 3D modeling ๋ฐฉ๋ฒ์ ๋ค์ํ ์ ํ์ ๋ค์์ ์์คํ
์ ๋ง์ถฐ์ ธ ์์ผ๋ฉฐ, ์ด๋ฅผ ํตํด ordered multi-element system๊ณผ disordered multi-element system์์ ์์์ ์์น๋ฅผ ํ์
ํ๊ณ ์์์ ์ข
๋ฅ๋ฅผ ๊ตฌ๋ถํ ์ ์๋ค. First-principles calculation์ ํตํด ์ป์ PbSe, CdSe, FePt ๋๋
ธ์
์ ๊ตฌ์กฐ๋ก๋ถํฐ ๊ทธ๋ํ ์ก์ฒด ์
์์์์ TEM ์๋ฎฌ๋ ์ด์
์ด๋ฏธ์ง๋ฅผ ์ป๊ณ , ์ด๋ฅผ ํ์ฉํ์ฌ ๊ตฌ์ฑ ์์์ ์ ํ๊ณผ ์์น๋ฅผ 24 ํผ์ฝ๋ฏธํฐ ๋ฏธ๋ง์ ์ค์ฐจ๋ก ์ ํ๋ ๋๊ฒ ํ๋ณํ ์ ์์์ ํ์ธํ์๋ค. ์ฐ๋ฆฌ์ ์ฐ๊ตฌ๋ ์ก์์์ ํฉ์ฑ๋ ๋ค์์ ๋๋
ธ์
์์ 3์ฐจ์ ์์ ๊ตฌ์กฐ๋ฅผ ์กฐ์ฌํ๋ ๊ฒ์ด ๊ฐ๋ฅํจ์ ์์ฌํ๋ค.Chapter 1. Introdution 1
1.1. Atomic structure property relationships in nanoparticles 1
1.2. Toward atomic structure characterization 2
1.3. Direct observation of 3D atomic structures of individual nanoparticles: Electron tomography and Brownian one-particle reconstruction 3
1.4. Purpose of Research 4
Chapter 2. 3D atomic structures of individual ligand-protected Pt nanoparticles in solution 7
2.1. Introduction 7
2.2. 3D reconstruction from electron microscopy images of Pt nanoparticles in liquid 8
2.2.1. Synthesis of Pt nanoparticles 8
2.2.2. Preparation of graphene liquid cells 9
2.2.3. Acquisition of TEM images 9
2.2.4. 3D reconstruction 10
2.2.5. Atomic position assignment 11
2.2.6. Validation 11
2.2.7. Atomic structure analysis 13
2.3. Atomic structural characteristics of Pt nanoparticles in liquid 16
2.2.1. Effect of surface ligands on the 3D atomic structures of Pt nanoparticles 16
2.3.2. Structural heterogeneity of Pt nanoparticles 18
2.3.3. Strain analysis of individual Pt nanoparticles from the 3D atomic maps 19
2.4. Conclusion 21
Chapter 3. SINGLE: Computational methods for atomic-resolution 3D reconstruction 57
3.1. Introduction 57
3.2. Results 58
3.2.1. Overview of 3D SINGLE 58
3.2.2. The SINGLE workflow 58
3.3. Conclusion 66
Chapter 4. 3-Dimensional scanning of unit cell symmetries in individual nanoparticles by using Brownian one-particle reconstruction 75
4.1. Introduction 75
4.2. Results 77
4.2.1. Quantitative symmetry analysis from 3D atomic coordinates 77
4.2.2. Direction of symmetry breakage 79
4.2.3. Structural heterogeneity 80
4.2.4. Relationship between symmetry and surface interactions 80
4.3. Conclusion 84
Chapter 5. Method for 3D atomic structure determination of multi-element nanoparticles with graphene liquid-cell TEM 102
5.1. Introduction 102
5.2. Results 104
5.2.1. Overview of multi-element nanoparticle 3D reconstruction 104
5.2.2. Principles for multi-element nanoparticle reconstruction 105
5.2.3. Demonstration using simulated TEM images 106
5.3. Conclusion 111
Bibliography 136
๊ตญ ๋ฌธ ์ด ๋ก 144๋ฐ
Recommended from our members
Improved methods for single-particle cryogenic electron microscopy
Biological macromolecules such as enzymes are nanoscale machines. This is true in a concrete sense: if the atomic structure of a biological macromolecule can be obtained, the theories of mechanics and intermolecular forces can be applied to explain how the machine works in terms that engineers would understand, including motors, ratchets, gates and transducers. Nevertheless, biological macromolecules are complex, fragile and extremely small, so obtaining their structures is a challenging experimental endeavor. Single-particle cryogenic electron microscopy (cryo-EM) is a technique for determining the 3D structure of a biological macromolecule from a large set of 2D electron micrographs of individual structurally-identical particles. To obtain such images, a solution of the macromolecules must be prepared in the frozen-hydrated state, embedded in a thin electron-transparent glassy film of water. This specimen must then be imaged with a very short exposure to avoid radiation damage. A powerful computer must then be used to sort, align, and average the 2D particle images to back-calculate the 3D structure. At its best, cryo-EM can determine the structures of biological macromolecules to atomic resolution. In practice, this goal is usually not achieved. Cryo-EM has gotten significantly more powerful in the past few years due to improvements in equipment and methodology. Several of the most significant advances originated in the labs of David Agard and Yifan Cheng at UCSF. When I began my PhD with Yifan, the spirit in the lab was that cryo-EM could keep getting better and better: with enough engineering, determining the 3D structure of an arbitrary biological macromolecule would be as routine an experiment as gel electrophoresis or DNA sequencing. Inspired, I took on projects in the lab that I thought would move the field closer to that goal. In the first chapter of this thesis, I describe work I did supporting a project initiated by David Agard and his long-time scientific programmer Shawn Zheng. They developed and implemented an algorithm, MotionCor2, for correcting the complex, anisotropic movements that occur when a frozen-hydrated specimen interacts with the high-energy electron beam. My role was to benchmark MotionCor2 on a panel of real-world 3D reconstruction tasks. I was able to show that MotionCor2 restored the highest resolution details in the images, ultimately yielding significantly better structures than simpler algorithms. For me, this projected highlighted the importance of benchmarking an algorithm for use in routine real-world conditions with the right metrics. In chapter 1, I include the manuscript for the MotionCor2 study, formatted to highlight my contributions that were moved to the supplement in the original publication by Nature Methods. One of the major remaining issues with cryo-EM is sample preparation: preparing the thin freestanding films of frozen-hydrated particles necessarily exposes those particles to air-water interfaces. Many fragile macromolecular complexes denature when exposed to such interfaces, preventing structure determination with cryo-EM. In chapters 2 and 3, I describe my efforts to develop a simple, robust approach to stabilizing fragile macromolecular complexes during the vitrification process. In chapter 2, I develop a method for coating EM grids with an electron-transparent and functionalizable graphene-oxide support film. I demonstrate that such GO grids are compatible with high-resolution structure determination. This work was published in the Journal of Structural Biology in 2018. In chapter 3, I extend this work by functionalizing GO grids with nucleic acids, enabling routine structure determination of uncrosslinked chromatin specimens. In on-going work, I used nucleic acid grids to solve high-resolution structures of a highly fragile specimen, the snf2h-nucleosome complex, and analyzed the conformational heterogeneity of the nucleosome substrate. These results were made possible by the nucleic acid grid, as the other major approach for stabilizing chromatin specimens, chemical crosslinking, not work for this specimen.Perhaps the most fundamental problem with single-particle cryo-EM is the radiation sensitivity of frozen-hydrated macromolecules. To image biological matter with electrons is to destroy it, so obtaining images of undamaged specimens requires very short, highly under sampled exposures. The resultant images are extremely noisy and low contrast, with most particles barely visible from the background. In chapter 4, I describe a novel computational approach to generating contrast in cryo-EM. Using a recently described machine learning strategy for training a parameterized denoising algorithm, I developed a computer program, restore, that denoises cryo-EM images, greatly enhancing their contrast and interpretability. This program leverages recent advances in computer vision and deep learning which have not yet been widely used in cryo-EM image processing algorithms. To characterize the performance of the algorithm on real-world data, I extended conventional metrics for image resolution to measure how an arbitrary transformation affects images at different spatial frequencies. These novel metrics are general and may be useful for characterizing other nonlinear reconstruction algorithms in cryo-EM and medical imaging. Finally, I showed that denoised cryo-EM images maintain the high-resolution information required for accurate 3D reconstruction. Denoising can be applied to conventional cryo-EM images and can be reversed whenever necessary. I have made the software for restore program publicly available and have submitted a manuscript for peer-reviewed publication
Correlated Multimodal Imaging in Life Sciences:Expanding the Biomedical Horizon
International audienceThe frontiers of bioimaging are currently being pushed toward the integration and correlation of several modalities to tackle biomedical research questions holistically and across multiple scales. Correlated Multimodal Imaging (CMI) gathers information about exactly the same specimen with two or more complementary modalities that-in combination-create a composite and complementary view of the sample (including insights into structure, function, dynamics and molecular composition). CMI allows to describe biomedical processes within their overall spatio-temporal context and gain a mechanistic understanding of cells, tissues, diseases or organisms by untangling their molecular mechanisms within their native environment. The two best-established CMI implementations for small animals and model organisms are hardware-fused platforms in preclinical imaging (Hybrid Imaging) and Correlated Light and Electron Microscopy (CLEM) in biological imaging. Although the merits of Preclinical Hybrid Imaging (PHI) and CLEM are well-established, both approaches would benefit from standardization of protocols, ontologies and data handling, and the development of optimized and advanced implementations. Specifically, CMI pipelines that aim at bridging preclinical and biological imaging beyond CLEM and PHI are rare but bear great potential to substantially advance both bioimaging and biomedical research. CMI faces three mai
Multireference Alignment is Easier with an Aperiodic Translation Distribution
In the multireference alignment model, a signal is observed by the action of
a random circular translation and the addition of Gaussian noise. The goal is
to recover the signal's orbit by accessing multiple independent observations.
Of particular interest is the sample complexity, i.e., the number of
observations/samples needed in terms of the signal-to-noise ratio (the signal
energy divided by the noise variance) in order to drive the mean-square error
(MSE) to zero. Previous work showed that if the translations are drawn from the
uniform distribution, then, in the low SNR regime, the sample complexity of the
problem scales as . In this work, using a
generalization of the Chapman--Robbins bound for orbits and expansions of the
divergence at low SNR, we show that in the same regime the sample
complexity for any aperiodic translation distribution scales as
. This rate is achieved by a simple spectral algorithm.
We propose two additional algorithms based on non-convex optimization and
expectation-maximization. We also draw a connection between the multireference
alignment problem and the spiked covariance model
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