417 research outputs found

    GENFIRE: A generalized Fourier iterative reconstruction algorithm for high-resolution 3D imaging

    Get PDF
    Tomography has made a radical impact on diverse fields ranging from the study of 3D atomic arrangements in matter to the study of human health in medicine. Despite its very diverse applications, the core of tomography remains the same, that is, a mathematical method must be implemented to reconstruct the 3D structure of an object from a number of 2D projections. In many scientific applications, however, the number of projections that can be measured is limited due to geometric constraints, tolerable radiation dose and/or acquisition speed. Thus it becomes an important problem to obtain the best-possible reconstruction from a limited number of projections. Here, we present the mathematical implementation of a tomographic algorithm, termed GENeralized Fourier Iterative REconstruction (GENFIRE). By iterating between real and reciprocal space, GENFIRE searches for a global solution that is concurrently consistent with the measured data and general physical constraints. The algorithm requires minimal human intervention and also incorporates angular refinement to reduce the tilt angle error. We demonstrate that GENFIRE can produce superior results relative to several other popular tomographic reconstruction techniques by numerical simulations, and by experimentally by reconstructing the 3D structure of a porous material and a frozen-hydrated marine cyanobacterium. Equipped with a graphical user interface, GENFIRE is freely available from our website and is expected to find broad applications across different disciplines.Comment: 18 pages, 6 figure

    Biological application of Compressed Sensing Tomography in the Scanning Electron Microscope

    Get PDF
    The three-dimensional tomographic reconstruction of a biological sample, namely collagen fibrils in human dermal tissue, was obtained from a set of projection-images acquired in the Scanning Electron Microscope. A tailored strategy for the transmission imaging mode was implemented in the microscope and proved effective in acquiring the projections needed for the tomographic reconstruction. Suitable projection alignment and Compressed Sensing formulation were used to overcome the limitations arising from the experimental acquisition strategy and to improve the reconstruction of the sample. The undetermined problem of structure reconstruction from a set of projections, limited in number and angular range, was indeed supported by exploiting the sparsity of the object projected in the electron microscopy images. In particular, the proposed system was able to preserve the reconstruction accuracy even in presence of a significant reduction of experimental projections

    Zernike Phase Contrast Cryo-Electron Microscopy and Tomography for Structure Determination at Nanometer and Subnanometer Resolutions

    Get PDF
    Zernike phase contrast cryo-electron microscopy (ZPC-cryoEM) is an emerging technique that is capable of producing higher image contrast than conventional cryoEM. By combining this technique with advanced image processing methods, we achieved subnanometer resolution for two biological specimens: 2D bacteriorhodopsin crystal and epsilon15 bacteriophage. For an asymmetric reconstruction of epsilon15 bacteriophage, ZPC-cryoEM can reduce the required amount of data by a factor of ~3, compared with conventional cryoEM. The reconstruction was carried out to 13 ร… resolution without the need to correct the contrast transfer function. New structural features at the portal vertex of the epsilon15 bacteriophage are revealed in this reconstruction. Using ZPC cryo-electron tomography (ZPC-cryoET), a similar level of data reduction and higher resolution structures of epsilon15 bacteriophage can be obtained relative to conventional cryoET. These results show quantitatively the benefits of ZPC-cryoEM and ZPC-cryoET for structural determinations of macromolecular machines at nanometer and subnanometer resolutions.National Institutes of Health (U.S.) (Grant P41RR002250)National Institutes of Health (U.S.) (Grant R01AI0175208)National Institutes of Health (U.S.) (Grant PN1EY016525)Robert Welch Foundation (Q1242

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

    Get PDF
    ํ•™์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•

    In situ structure of virus capsids within cell nuclei by correlative light and cryo-electron tomography

    Get PDF
    Cryo electron microscopy (cryo-EM), a key method for structure determination involves imaging purified material embedded in vitreous ice. Images are then computationally processed to obtain three-dimensional structures approaching atomic resolution. There is increasing interest in extending structural studies by cryo-EM into the cell, where biological structures and processes may be imaged in context. The limited penetrating power of electrons prevents imaging of thick specimens (>โ€‰500 nm) however. Cryo-sectioning methods employed to overcome this are technically challenging, subject to artefacts or involve specialised and costly equipment. Here we describe the first structure of herpesvirus capsids determined by sub-tomogram averaging from nuclei of eukaryotic cells, achieved by cryo-electron tomography (cryo-ET) of re-vitrified cell sections prepared using the Tokuyasu method. Our reconstructions confirm that the capsid associated tegument complex is present on capsids prior to nuclear egress. We demonstrate that this method is suited to both 3D structure determination and correlative light/electron microscopy, thus expanding the scope of cryogenic cellular imaging

    Automatic Differentiation for Inverse Problems in X-ray Imaging and Microscopy

    Get PDF
    Computational techniques allow breaking the limits of traditional imaging methods, such as time restrictions, resolution, and optics flaws. While simple computational methods can be enough for highly controlled microscope setups or just for previews, an increased level of complexity is instead required for advanced setups, acquisition modalities or where uncertainty is high; the need for complex computational methods clashes with rapid design and execution. In all these cases, Automatic Differentiation, one of the subtopics of Artificial Intelligence, may offer a functional solution, but only if a GPU implementation is available. In this paper, we show how a framework built to solve just one optimisation problem can be employed for many different X-ray imaging inverse problems
    • โ€ฆ
    corecore