2,106 research outputs found

    Numerical Geometry of Map and Model Assessment

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    We are describing best practices and assessment strategies for the atomic interpretation of cryo-electron microscopy (cryo-EM) maps. Multiscale numerical geometry strategies in the Situs package and in secondary structure detection software are currently evolving due to the recent increases in cryo-EM resolution. Criteria that aim to predict the accuracy of fitted atomic models at low (worse than 8 angstrom) and medium (4-8 angstrom) resolutions remain challenging. However, a high level of confidence in atomic models can be achieved by combining such criteria. The observed errors are due to map-model discrepancies and due to the effect of imperfect global docking strategies. Extending the earlier motion capture approach developed for flexible fitting, we use simulated fiducials (pseudoatoms) at varying levels of coarse-graining to track the local drift of structural features. We compare three tracking approaches: naive vector quantization, a smoothly deformable model, and a tessellation of the structure into rigid Voronoi cells, which are fitted using a multi-fragment refinement approach. The lowest error is an upper bound for the (small) discrepancy between the crystal structure and the EM map due to different conditions in their structure determination. When internal features such as secondary structures are visible in medium-resolution EM maps, it is possible to extend the idea of point-based fiducials to more complex geometric representations such as helical axes, strands, and skeletons. We propose quantitative strategies to assess map-model pairs when such secondary structure patterns are prominent

    Conformational states of macromolecular assemblies explored by integrative structure calculation

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    A detailed description of macromolecular assemblies in multiple conformational states can be very valuable for understanding cellular processes. At present, structural determination of most assemblies in different biologically relevant conformations cannot be achieved by a single technique and thus requires an integrative approach that combines information from multiple sources. Different techniques require different computational methods to allow efficient and accurate data processing and analysis. Here, we summarize the latest advances and future challenges in computational methods that help the interpretation of data from two techniquesโ€”mass spectrometry and three-dimensional cryo-electron microscopy (with focus on alignment and classification of heterogeneous subtomograms from cryo-electron tomography). We evaluate how new developments in these two broad fields will lead to further integration with atomic structures to broaden our picture of the dynamic behavior of assemblies in their native environment

    Expansion-enhanced super-resolution radial fluctuations enable nanoscale molecular profiling of pathology specimens

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    Expansion microscopy physically enlarges biological specimens to achieve nanoscale resolution using diffraction-limited microscopy systems1. However, optimal performance is usually reached using laser-based systems (for example, confocal microscopy), restricting its broad applicability in clinical pathology, as most centres have access only to light-emitting diode (LED)-based widefield systems. As a possible alternative, a computational method for image resolution enhancement, namely, super-resolution radial fluctuations (SRRF)2,3, has recently been developed. However, this method has not been explored in pathology specimens to date, because on its own, it does not achieve sufficient resolution for routine clinical use. Here, we report expansion-enhanced super-resolution radial fluctuations (ExSRRF), a simple, robust, scalable and accessible workflow that provides a resolution of up to 25 nm using LED-based widefield microscopy. ExSRRF enables molecular profiling of subcellular structures from archival formalin-fixed paraffin-embedded tissues in complex clinical and experimental specimens, including ischaemic, degenerative, neoplastic, genetic and immune-mediated disorders. Furthermore, as examples of its potential application to experimental and clinical pathology, we show that ExSRRF can be used to identify and quantify classical features of endoplasmic reticulum stress in the murine ischaemic kidney and diagnostic ultrastructural features in human kidney biopsies.</p

    Normal Mode Flexible Fitting of High-Resolution Structures of Biological Molecules Toward SAXS Data

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    We present a method to reconstruct a three-dimensional protein structure from an atomic pair distribution function derived from the scattering intensity profile from SAXS data by flexibly fitting known x-ray structures. This method uses a linear combination of low-frequency normal modes from an elastic network description of the molecule in an iterative manner to deform the structure to conform optimally to the target pair distribution function derived from SAXS data. For computational efficiency, the protein and water molecules included in the protein first hydration shell are coarse-grained. In this paper, we demonstrate the validity of our coarse-graining approach to study SAXS data. Illustrative results of our flexible fitting studies on simulated SAXS data from five different proteins are presented

    Improved biological annotation of EMDB data

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    Curs 2015-2016In this Final degree Project are explained all processes required to create the segmentation and biological annotation parts of Segmentation File Format (SFF) project. The segmentation file format is an Electron Microscope Data Base (EMDB) project, which is a combination of two projects, the โ€œOMERO volume slicerโ€ and the โ€œSegmentation annotation toolโ€. This project was developed in order to build the segmentation and annotation sets for the โ€œSegmentation annotation toolโ€ step. The project was divided into two steps, Segmentation using Chimera, that permitted the downloading of the EMDB and PDB structure and proceed to do the segmentation, then this segmentation was saved as an Segger or HDF5 file. The segmentation of a structure is the decomposition by the different components that forms it. The second part consisted to create a biological annotation of the components previously segmented and building a link with other databases in order to identify them. The objective of this project was to create a SFF, this application would permit to the user to visualize segmentations on a EM tomogram, in order to identify and distinguish all the components that composed it. The annotation and segmentation that is explained in this project was made as a data set to build this new EMDB application. On the end of the project a collection of 100 segmentation and annotation sets were obtained, three types of structures can be distinguished; Helicases, Chaperones and Ribosomes

    Ball-and-chain inactivation in a calcium-gated potassium channel

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    Inactivation is the process by which ion channels terminate ion flux through their pores while the opening stimulus is still present1. In neurons, inactivation of both sodium and potassium channels is crucial for the generation of action potentials and regulation of firing frequency1,2. A cytoplasmic domain of either the channel or an accessory subunit is thought to plug the open pore to inactivate the channel via a โ€˜ball-and-chainโ€™ mechanism3โ€“7. Here we use cryo-electron microscopy to identify the molecular gating mechanism in calcium-activated potassium channels by obtaining structures of the MthK channel from Methanobacterium thermoautotrophicumโ€”a purely calcium-gated and inactivating channelโ€”in a lipid environment. In the absence of Ca2+, we obtained a single structure in a closed state, which was shown by atomistic simulations to be highly flexible in lipid bilayers at ambient temperature, with large rocking motions of the gating ring and bending of pore-lining helices. In Ca2+-bound conditions, we obtained several structures, including multiple open-inactivated conformations, further indication of a highly dynamic protein. These different channel conformations are distinguished by rocking of the gating rings with respect to the transmembrane region, indicating symmetry breakage across the channel. Furthermore, in all conformations displaying open channel pores, the N terminus of one subunit of the channel tetramer sticks into the pore and plugs it, with free energy simulations showing that this is a strong interaction. Deletion of this N terminus leads to functionally non-inactivating channels and structures of open states without a pore plug, indicating that this previously unresolved N-terminal peptide is responsible for a ball-and-chain inactivation mechanism

    ์•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•

    Geometric analysis of macromolecule organization within cryo-electron tomograms

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    Cryo-electron tomography (CET) provides unprecedented views into the native cellular environment at molecular resolution. While subtomogram analysis yields high-resolution native structures of molecular complexes, it also determines the precise positions and orientations of these macromolecules within the cell. Analyzing the geometric relationships between adjacent macromolecules can offer structural insights into molecular interactions and identify supramolecular ensembles. However, computation..
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