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    Fast and robust single particle reconstruction in 3D fluorescence microscopy

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    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

    ์•ก์ƒ์— ์กด์žฌํ•˜๋Š” ๊ฐœ๋ณ„ ๋‚˜๋…ธ์ž…์ž์— ๋Œ€ํ•œ 3์ฐจ์› ์›์ž๊ตฌ์กฐ ๋ถ„์„ ๋ฐฉ๋ฒ•๋ก 

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2023. 2. ๋ฐ•์ •์›.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 cryoโ€“electron 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.์žฌ๋ฃŒ์˜ 3D ์›์ž ๋ฐฐ์—ด์ด ์ž์œ  ์—๋„ˆ์ง€ ํ™˜๊ฒฝ์„ ๊ฒฐ์ •ํ•œ๋‹ค๋Š” ์ ์„ ๊ณ ๋ คํ–ˆ์„ ๋•Œ, ๊ฐœ๋ณ„ ๋‚˜๋…ธ๊ฒฐ์ •์˜ ์ •ํ™•ํ•œ 3์ฐจ์›(3D) ์›์ž ๊ตฌ์กฐ ๋ถ„์„์€ ๋ฌผ๋ฆฌ์  ํŠน์„ฑ์„ ์ดํ•ดํ•˜๊ณ  ์˜ˆ์ธกํ•˜๊ธฐ ์œ„ํ•ด ํ•„์ˆ˜ ๋ถˆ๊ฐ€๊ฒฐํ•˜๋‹ค. ๋ณธ ์—ฐ๊ตฌ์ž๋Š” ๊ทธ๋ž˜ํ•€ ์•ก์ฒด ์„ธํฌ ํˆฌ๊ณผ ์ „์ž ํ˜„๋ฏธ๊ฒฝ์„ ์‚ฌ์šฉํ•˜์—ฌ ์ฝœ๋กœ์ด๋“œ ๋‚˜๋…ธ์ž…์ž์˜ ์•™์ƒ๋ธ” ์ด๋ฏธ์ง•์„ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•˜๋Š” "๋ธŒ๋ผ์šด ๋‹จ์ผ ์ž…์ž ์žฌ๊ตฌ์„ฑ"์„ ๊ฐœ๋ฐœํ–ˆ๋‹ค. ๋™์ผํ•œ ํ•ฉ์„ฑ ๋ฐฐ์น˜์˜ ๋‚˜๋…ธ์ž…์ž๋Š” ํฌ๊ธฐ, ๊ฒฉ์ž ์™œ๊ณก ๋ฐ ๊ฒฐํ•จ ๋“ฑ์—์„œ ์ข…์ข… ์ž‘์ง€๋งŒ ์ค‘์š”ํ•œ ๊ฒƒ์œผ๋กœ ์ถ”์ •๋˜๋Š” ๊ฒƒ์œผ๋กœ ๊ฐ„์ฃผ๋˜๋Š” ๊ตฌ์กฐ์  ์ฐจ์ด์ ์ด ์žˆ์œผ๋ฉฐ, ์ด๋Š” 3D ๊ณ ํ•ด์ƒ๋„ ๊ตฌ์กฐ ๋ถ„์„์— ์˜ํ•ด์„œ๋งŒ ์ดํ•ดํ•  ์ˆ˜ ์žˆ๋‹ค. ๊ตฌ์กฐ์  ํ‡ดํ™”, ๊ฒฉ์ž ๋งค๊ฐœ๋ณ€์ˆ˜ ํŽธ์ฐจ, ๋‚ด๋ถ€ ๊ฒฐํ•จ ๋ฐ ๋ณ€ํ˜•์„ ํฌํ•จํ•œ ๊ฐœ๋ณ„ ์ฝœ๋กœ์ด๋“œ ๋ฐฑ๊ธˆ ๋‚˜๋…ธ์ž…์ž์˜ ๊ตฌ์กฐ์  ํŠน์„ฑ์€ ์›์ž ๋ถ„ํ•ด๋Šฅ 3D ์•ก์ฒด ์„ธํฌ ์ „์ž ํ˜„๋ฏธ๊ฒฝ์„ ๊ฐœ๋ฐœํ•˜์—ฌ ํ’€์–ด๋‚ผ ์ˆ˜ ์žˆ๋‹ค. ์ด๋Ÿฌํ•œ ๊ตฌ์กฐ์˜ ์ฐจ์ด๋Š” ์ž์œ  ์—๋„ˆ์ง€์— ์ƒ๋‹นํ•œ ๊ธฐ์—ฌ๋ฅผ ํ•˜๋ฏ€๋กœ ๊ฒฐ๊ณผ์ ์œผ๋กœ ๊ธฐ๋ณธ์ ์ธ ๋‚˜๋…ธ์ž…์ž ํŠน์„ฑ ๋˜๋Š” ์‘์šฉ์— ๋Œ€ํ•œ ๋…ผ์˜์—์„œ ๊ณ ๋ ค๋˜์–ด์•ผ ํ•œ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์„ฑ๊ณต์ ์ธ ์›์ž ํ•ด์ƒ๋„ 3D ์žฌ๊ตฌ์„ฑ์— ํ•„์š”ํ•œ ๊ณ„์‚ฐ ๋ฐฉ๋ฒ•๋ก ์„ ์†Œ๊ฐœํ•œ๋‹ค. ๊ทธ ๋ฐฉ๋ฒ•๋ก ์—๋Š” ๋‹ค์Œ๊ณผ ๊ฐ™์€ ์•Œ๊ณ ๋ฆฌ์ฆ˜์ด ํฌํ•จ๋œ๋‹ค. (1) ์‹œ๊ณ„์—ด ์ด๋ฏธ์ง€์—์„œ ๊ฐœ๋ณ„ ๋‚˜๋…ธ์ž… ์ž๋ฅผ ์ถ”์ ํ•˜๋Š” ์•Œ๊ณ ๋ฆฌ์ฆ˜, (2) ๊ทธ๋ž˜ํ•€ ์•ก์ฒด ์…€์˜ ๋ฐฐ๊ฒฝ ๋…ธ์ด์ฆˆ๋ฅผ ์ œ๊ฑฐํ•˜๋Š” ์•Œ๊ณ ๋ฆฌ์ฆ˜, (3) ์ €ํ•ด์ƒ๋„ ์ด๋ฏธ์ง€๋ฅผ ๊ฒ€์ถœ ๋ฐ ์ œ๊ฑฐํ•˜๋Š” ์•Œ๊ณ ๋ฆฌ์ฆ˜, (4) ๊ทน์ €์˜จ ์ „์žํ˜„๋ฏธ๊ฒฝ์„ ์ด์šฉํ•œ ๋ฐ”์ด์˜ค ์ž…์ž์˜ ์žฌ๊ตฌ์„ฑ์— ์“ฐ์ด๋Š” ์•Œ๊ณ ๋ฆฌ์ฆ˜๊ณผ๋Š” ๋‹ค๋ฅธ ๋‚˜๋…ธ์ž…์ž๋งŒ์„ ์œ„ํ•ด์„œ ๊ณ ์•ˆ๋œ 2์ฐจ์›/3์ฐจ์› ์ •๋ ฌ ์•Œ๊ณ ๋ฆฌ์ฆ˜. ๊ฒฉ์ž ๋Œ€์นญ์„ฑ์€ ๋‚˜๋…ธ ๋ฌผ์งˆ์˜ ๋ฌผ๋ฆฌ์  ํŠน์„ฑ๊ณผ ๊ฐ•ํ•œ ์ƒ๊ด€๊ด€๊ณ„๊ฐ€ ์žˆ๊ธฐ ๋•Œ๋ฌธ์—, ๊ฒฉ์ž ๋Œ€์นญ์„ฑ ๋ถ„์„์€ ์ค‘์š”ํ•˜๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์•ก์ƒ ํˆฌ๊ณผ ์ „์ž ํ˜„๋ฏธ๊ฒฝ์„ ํ†ตํ•ด์„œ ์–ป์€ 3์ฐจ์› ์›์ž ์ขŒํ‘œ๋ฅผ ์ด์šฉํ•˜์—ฌ ๊ฒฉ์ž ๋Œ€์นญ์„ ์ง์ ‘์ , ์ •๋Ÿ‰์ ์œผ๋กœ ๋ถ„์„ํ•  ์ˆ˜ ์žˆ๋Š” ๋ฐฉ๋ฒ•๋ก ์„ ์†Œ๊ฐœํ•˜๊ณ ์ž ํ•œ๋‹ค. ๊ฐœ๋ณ„ ๋ฐฑ๊ธˆ ๋‚˜๋…ธ์ž…์ž๋ฅผ ๊ตฌ์„ฑํ•˜๋Š” ์ „์ฒด unit cell์˜ ๋Œ€์นญ์„ฑ์„ ์กฐ์‚ฌํ•จ์œผ๋กœ์จ, 3 ๋‚˜๋…ธ๋ฏธํ„ฐ ์ดํ•˜์˜ ๋ฐฑ๊ธˆ ๋‚˜๋…ธ์ž…์ž๊ฐ€ ๊ฐ–๋Š” ๋…ํŠนํ•œ ๊ตฌ์กฐ์  ํŠน์ง•์„ ๋ฐํ˜€๋‚ด์˜€๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๋‹ค์›์†Œ ๋‚˜๋…ธ์ž…์ž ์‹œ์Šคํ…œ์„ ์œ„ํ•œ 3์ฐจ์› ์›์ž ๊ตฌ์กฐ ๋ถ„์„๋ฒ•์„ ์†Œ๊ฐœํ•˜๊ณ ์ž ํ•œ๋‹ค. ์ œ์‹œ๋œ low-pass filtering๊ณผ initial 3D modeling ๋ฐฉ๋ฒ•์€ ๋‹ค์–‘ํ•œ ์œ ํ˜•์˜ ๋‹ค์›์†Œ ์‹œ์Šคํ…œ์— ๋งž์ถฐ์ ธ ์žˆ์œผ๋ฉฐ, ์ด๋ฅผ ํ†ตํ•ด ordered multi-element system๊ณผ disordered multi-element system์—์„œ ์›์ž์˜ ์œ„์น˜๋ฅผ ํŒŒ์•…ํ•˜๊ณ  ์›์†Œ์˜ ์ข…๋ฅ˜๋ฅผ ๊ตฌ๋ถ„ํ•  ์ˆ˜ ์žˆ๋‹ค. First-principles calculation์„ ํ†ตํ•ด ์–ป์€ PbSe, CdSe, FePt ๋‚˜๋…ธ์ž…์ž ๊ตฌ์กฐ๋กœ๋ถ€ํ„ฐ ๊ทธ๋ž˜ํ•€ ์•ก์ฒด ์…€ ์•ˆ์—์„œ์˜ TEM ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ์ด๋ฏธ์ง€๋ฅผ ์–ป๊ณ , ์ด๋ฅผ ํ™œ์šฉํ•˜์—ฌ ๊ตฌ์„ฑ ์›์ž์˜ ์œ ํ˜•๊ณผ ์œ„์น˜๋ฅผ 24 ํ”ผ์ฝ”๋ฏธํ„ฐ ๋ฏธ๋งŒ์˜ ์˜ค์ฐจ๋กœ ์ •ํ™•๋„ ๋†’๊ฒŒ ํŒ๋ณ„ํ•  ์ˆ˜ ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์šฐ๋ฆฌ์˜ ์—ฐ๊ตฌ๋Š” ์•ก์ƒ์—์„œ ํ•ฉ์„ฑ๋œ ๋‹ค์›์†Œ ๋‚˜๋…ธ์ž…์ž์˜ 3์ฐจ์› ์›์ž ๊ตฌ์กฐ๋ฅผ ์กฐ์‚ฌํ•˜๋Š” ๊ฒƒ์ด ๊ฐ€๋Šฅํ•จ์„ ์‹œ์‚ฌํ•œ๋‹ค.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 ์ดˆ ๋ก 144๋ฐ•

    Correlated Multimodal Imaging in Life Sciences:Expanding the Biomedical Horizon

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    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

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    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 ฯ‰(1/SNR3)\omega(1/\text{SNR}^3). In this work, using a generalization of the Chapman--Robbins bound for orbits and expansions of the ฯ‡2\chi^2 divergence at low SNR, we show that in the same regime the sample complexity for any aperiodic translation distribution scales as ฯ‰(1/SNR2)\omega(1/\text{SNR}^2). 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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