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666 results for “Diffraction”
Raw diffraction images of YidC (phasing data by Hg-MAD)
<p>Diffraction images of mercury-bound <em>Bacillus halodurans</em> YidC mutants for Hg-MAD phasing. This phase information was used for PDB entries <a href="http://www.pdb.org/pdb/search/structidSearch.do?structureId=3WO6">3WO6</a> and <a href="http://www.pdb.org/pdb/search/structidSearch.do?structureId=3WO7">3WO7</a> (<a href="https://doi.org/10.1038/nature13167">Kumazaki et al. 2014</a>). All data were collected from loop-harvested crystals on BL32XU, SPring-8 at wavelengths of 1.00000 Å (peak) or 1.00945 Å (edge) using the MX225HE CCD detector.</p> <p>From the M146C mutant, helical (360 or 720°/crystal, 2°/frame) datasets were collected using 10×1 μm<sup>2</sup> beam. From a Y150C mutant, a helical (360°/crystal, 2.5°/frame) dataset was collected using 15×1 μm<sup>2</sup> beam, which was used for phase determination. The crystals belonged to space group <em>P</em>2<sub>1</sub> with unit cell parameter a~44, b~60, c~60 Å, β~100°.</p>
Raw diffraction images of H+/Ca2+ exchanger CAX (phasing data by Hg-MAD)
<p>Diffraction images of mercury-bound H<sup>+</sup>/Ca<sup>2+</sup> exchanger from <em>Archaeoglobus fulgidus</em>. This phase information was used for a PDB entry <a href="https://www.rcsb.org/structure/4KPP">4KPP</a> (<a href="http://science.sciencemag.org/content/341/6142/168">Nishizawa et al. 2013</a>). All data were collected from loop-harvested crystals on BL32XU, SPring-8 at wavelengths of 1.00000 Å (peak), 1.00930 Å (edge), or 1.01300 Å (low remote) using the MX225HE CCD detector.</p> <p>From a mercury-derivatised crystal, helical (360°/crystal, 1°/frame) datasets were collected using 5×1 μm<sup>2</sup> beam. The crystal belonged to space group <em>P</em>2<sub>1</sub> with unit cell parameter a~64, b~98, c~72 Å, β~99°.</p>
Raw diffraction images of prokaryotic peptide transporter PepTSo2
<p>Diffraction images of prokaryotic peptide transporter PepTSo2. In Nagamura et al. (<a href="https://doi.org/10.1107/S2053230X19003546">Acta Cryst. F, 2019</a>), the crystal form A (PDB code: <a href="http://www.rcsb.org/structure/6JKD">6JKD</a>, space group I4, 3.9 Å resolution) and the form B (PDB code: <a href="http://www.rcsb.org/structure/6JKC">6JKC</a>, space group P42<sub>1</sub>2, 3.5 Å resolution) were reported.</p> <p>Small-wedge (5 or 10°/crystal) datasets collected from loop-harvested microcrystals using EIGER X 9M detector at a wavelength of 1 Å on BL32XU, SPring-8.</p> <p>PepT-So2_171220_BL32XU_{1..4}.tar.xz contains directories 01, 07-1, 07-2, 09, 10, 11. PepT-So2_180215_BL32XU.tar.xz contains directories 01, 02, 03, 04, 05, 14. Different directories are from different crystallization conditions. It seems they have different space groups even though they may share the same reduced cells. In the literature for form A data (I4, a=b=115, c=110 Å) from 07-2 and 11 of 171220_BL32XU were used while for form B data (P42<sub>1</sub>2, a=b=119, c=104.3 Å) from 04 and 05 of 180215_BL32XU were used.<br> <br> Note that master.h5 files were modified; see <a href="https://github.com/keitaroyam/yamtbx/blob/master/doc/eiger-en.md">https://github.com/keitaroyam/yamtbx/blob/master/doc/eiger-en.md</a>.</p>
Raw and processed anomalous diffraction data for crystals of metal-free R2lox soaked with Mn, Fe and Co or Zn
<p>Raw and processed anomalous diffraction data for crystals of metal-free <em>Geobacillus kaustophilus</em> R2-like ligand-binding oxidase (R2lox) soaked with 5 mM each MnCl<sub>2</sub>, (NH<sub>4</sub>)<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub> and CoCl<sub>2</sub> or ZnCl<sub>2</sub>. Data were collected on two crystals each after soaking with Mn, Fe and Co or Mn, Fe and Zn, respectively. For each crystal, one dataset each was collected at the Fe K edge (7162 eV), Mn K edge (6589 eV) and Co K edge (7721 eV) or Zn K edge (9664 eV; X-ray energies corresponding to the theoretical K edge + 50 eV). Data were collected at 100 K on a Pilatus 6M detector at beamline X06SA of the Swiss Light Source (SLS, Villigen, Switzerland) on September 23, 2012, and processed with XDS and XSCALE. All raw and processed diffraction data for each crystal are compressed into one file. </p>
SNase Diffraction Data and Analysis
<p>This upload contains data and analysis scripts used in the manuscript "Towards computational design of improved protein crystal resolution". In this dataset, Figures 3 and 9 can be generated using the analyze_xscale.R script; source data for Figures 4, 5, and 6 can be found in the convert-map-for-pymol/ subdirectories; Figure 8 can be generated using the "plot_crystal_scores.R" script.</p>
Dataset for strain-localisation in helium implanted tungsten: CPFE, Laue diffraction, AFM
<p>The folder includes dataset for helium-implanted tungsten and pure tungsten. The data includes measurement of the following for both materials as observed experimentally, and predicted using crystal-plasticity simulations:</p> <p>1. Surface morphology of nano-indents,</p> <p>2. Lattice-distortions around and under nano-indents</p> <p>3. Computed geometrically necessary dislocations field around and under nano-indents in both materials</p> <p>4. Load-displacement curves</p> <p>Guidelines for using dataset:</p> <p>1. Extracting the folder will generate five individual folders</p> <p>2. In the AFM plots folder, use the matlab code and dataset in the the folder to generate the surface morphology of nano-indents.</p> <p>3. In the "CPFE implanted sample data" folder --> use "CPFE implanted matlab code" --> load "variables2" --> run the code (raw data is also provided in the folder)</p> <p>4. In the "CPFE unimplanted sample data" folder --> use "CPFE unimp matlab code" --> load "variables3" --> run the code (raw data is also provided in the folder)</p> <p>5. In the "Laue unimplanted data" folder --> use matlab code with relevant raw data provided in folder</p> <p>6. In the "Laue implanted data" folder --> use matlab code with relevant raw data provided in folder</p> <p>7. Excel sheet provides nano-indentation and CPFE predictions of load-displacement curves</p> <p>8. The folder "HR-EBSD code and data" includes related raw data and codes.</p>
Raw diffraction images of human ETB receptor in complex with IRL2500
<p>Crystal structure of the thermostabilized human ETB receptor in complex with peptide inverse agonist IRL2500 (PDB code: <a href="https://www.rcsb.org/structure/6K1Q">6K1Q</a>).</p> <p>Small-wedge (5-10°/crystal) datasets collected from loop-harvested microcrystals using <a href="https://github.com/keitaroyam/yamtbx/blob/master/doc/eiger-en.md">EIGER</a> X 9M detector at a wavelength of 1 Å on BL32XU, SPring-8. Beam size was around 10×10 µm<sup>2</sup> and oscillation step was 0.1°. The crystals belonged to space group I422 with unit cell parameters a=b~110, c~292 Å.</p> <p>In total 441 datasets were collected, and of these 428 datasets were indexed and integrated using XDS with <a href="https://github.com/keitaroyam/yamtbx/blob/master/doc/kamo-en.md">KAMO</a> pipeline. 88 integrated results were manually selected and finally 58 were merged at 2.6 Å resolution after CC-based clustering and outlier rejection by KAMO in the published result (<a href="https://doi.org/10.1038/s42003-019-0482-7">Nagiri et al. Communications Biology, 2019</a>).</p>
Crystal structure of olive flounder [Paralichthys olivaceus] interferon gamma at 2.3 Angstrom resolution - diffraction data
<p>Diffraction images, Bessy II (Berlin), MX 14.1, 12.5.2017, PDB ID 6F1E</p>
Scanning precession electron diffraction data of partly overlapping magnesium oxide nanoparticles
<p>Scanning precession electron diffraction (SPED) data of cubical magnesium oxide (MgO) nanoparticles are provided. The MgO particles in the data are partly overlapping and some share the same orientation. The dataset was used for demonstration of nanocrystal segmentation in SPED data, which is presented in the article entitled "Nanocrystal segmentation in scanning precession electron diffraction data" [1]. In this publication, two methods for nanocrystal segmentation are presented based on; i) virtual dark-field imaging and ii) non-negative matrix factorisation, both incorporating watershed image segmentation. The workflows and code used for the segmentation demonstrated in the article are available open-source [2].</p> <p>Here, two files are provided based on one raw SPED dataset:</p> <p>- "SPED_MgO_1.hdf5": raw data cropped in navigation space to dimensions (219, 228|144, 144) and exported to hdf5, and</p> <p>- "SPED_MgO.hdf5": the same data binned by 2 in navigation space to yield dimensions (109, 114|144, 144).</p> <p>Adrian Lervik is acknowledged for specimen preparation.</p> <p>[1] Bergh, T., Johnstone, D., Crout, P., Høgås, S., Midgley, P., Holmestad, R., Vullum, P. And Van Helvoort, A. (2019), Nanocrystal segmentation in scanning precession electron diffraction data. Journal of Microscopy. doi:<a href="https://doi.org/10.1111/jmi.12850">10.1111/Jmi.12850</a></p> <p>[2] Duncan N. Johnstone, Phillip Crout, Simon Høgås, Tina Bergh, Joonatan Laulainen, & Stef Smeets. (2019). pyxem/pyxem-demos: pyxem-demos v0.10.0. Zenodo. http://doi.org/10.5281/zenodo.3533670</p> <p> </p>
BIR-MicroED: TEM image series revealing bend contour motion in static microcrystals (biotin, Zn(II)-methionine, Co(II)-porphyrin, AVAAGA) and diffraction patterns acquired from the same crystals at 200 kV
<p>This deposition contains a series zip files each containing TEM image series and electron diffraction images in .mrc file format. Each folder collects data acquired from crystals of a particular compound under the same conditions (electron energy, temperature). Zip files are named according to the format: <em>"CompoundName</em>_bendcontour_imageseries_<em>AcceleratingVoltage</em>_<em>Temperature</em>.zip"</p> <p>Data is further divided into sub-directories according to the particular crystal studied (crystal1, crystal2, crystal3), each containing a TEM image series (name format: "<em>CompoundName</em>_static_imageseries_<em>AcceleratingVoltage</em>_<em>Temperature</em>_crystal#.mrc") and 10 diffraction snapshots (2 frames each, each convering 1 second of electron beam exposure) acquired at equally spaced time intervals throughout the image series. These are named according to the format:</p> <p>"CompoundName_bendcontour_crystal#_diffraction_snap#.mrc"</p>
Data for the publication "Hydrogen penetration into the NiTi superelastic alloy investigated in-situ by synchrotron diffraction experiments"
<p>This dataset contains the data to the research paper "Hydrogen penetration into the NiTi superelastic alloy investigated in-situ by synchrotron diffraction experiments". The paper describes a<span> microstructural evolution caused by a hydrogen permeation into the NiTi superelastic alloy, which was investigated in-situ using the X-ray synchrotron diffraction. The diffraction data, electrochemical data, TEM pictures, lattice parameters for ab-initio DFT calculations and input parametrs for FEM calculations are included.</span></p>
Residual stress in steel benchmark determined by synchrotron X-ray and neutron diffraction
<p>The data presented is the residual stress, determined by synchrotron X-ray diffraction (SXRD) at DESY operated by Hereo (P07 and P61A) and neutron diffraction (ND) at ILL(SALSA). The data is for two benchmark samples having the same geometry (U shape) that can be measured by diffraction techniques and adapted to other material systems to validate RS measurements. One of them was elastically loaded while the other had stresses generated by plastic deformation, while having the same geometry. </p> <p>The U-flexure sample flexure-compression(FC), flexure-tension(FT_ and flexure-neutral(FN) were electrical discharge machine from a rolled plate. The U-bend(B) sample was obtained by three-point bending a cuboidal blank. The thicknes of the machine part is close to 10 mm and runs parallel to the z-direction. The measurement line runs from the centre of the top surface near the bend (defined at the origin) down into the bend (positive z-direction). The FN samples acted as stress-free reference for the U-flexures and a pin extracted from the bend was used for the U-bend. For the U-flexures, a finite element analysis (FEA) model was developed to account for the slight variations in loading conditions observed in the samples used for ND and SXRD. The results of the FEA model is also presented for comparison.</p> <p>The gauge volume sizes and shapes were dependent on the technique and research facility. The gauge volumes were: a) P07 – 0.2 x 0.2 x ~2.0 mm<sup>3 </sup>(b) P61A- 0.15 x 0.15 x ~3.4 µm<sup>3 </sup>(c) SALSA- 0.6 x 0.6 x 2 mm<sup>3</sup>. </p>
RODIN X-ray Diffraction Data 2334961
<p>This dataset is part of the Resource of Diffraction Images Newcastle (RODIN), intended for the teaching of crystallography. More information about RODIN can be found on the <a title="Link to RODIN webpage on CCDC website" href="https://www.ccdc.cam.ac.uk/community/education-and-outreach/education/rodin/" target="_blank" rel="noopener">CCDC website</a>, as well as in the following article: </p> <p>J. Chem. Educ. 2024, 101, 10, 4276–4281 DOI: <a href="https://doi.org/10.1021/acs.jchemed.4c00797">10.1021/acs.jchemed.4c00797</a> </p> <p>RODIN was created for educational purposes and is ideal for teaching at secondary school and University level. We also encourage its use for teaching early-stage researchers crystallographic data processing and training new diffractometer users. The diffraction images from this project can be downloaded from Zenodo and used in teaching. You can use this resource to help students understand how to go from diffraction images to a solved crystal structure. Please note that structures from these datasets are already in the Cambridge Structural Database (CSD) and you should not submit your final structure solution to the CSD or publish them, they are intended for teaching purposes only. The diffraction images are provided under a CC-BY license. </p> <p>The zip file contains X-ray diffraction images for 1-phenyl-3,3-bis(phenylsulfanyl)prop-2-en-1-one collected for a crystal exhibiting non-merohedral twinning. A final structure solution for this data can be found in the CSD. This structure is published in the CSD as a CSD Communication and data shared with permission of the authors: Roly J. Armstrong, Aaron D. G. Campbell, Paul G. Waddell, CSD Communication, 2024</p> <p>The tables below summarise the data collection parameters for the experiment.</p> <p> </p> <p><strong>General information</strong></p> <table> <tbody> <tr> <td> <p>Project</p> </td> <td> <p>Repository of Diffraction Images Newcastle (RODIN)</p> </td> </tr> <tr> <td> <p>Collection Site</p> </td> <td> <p>Newcastle University, UK</p> </td> </tr> <tr> <td> <p>Sample Label</p> </td> <td> <p>rja230015_2</p> </td> </tr> <tr> <td> <p>Linked CCDC number</p> </td> <td> <p>2334961</p> </td> </tr> <tr> <td> <p>CSD Refcode</p> </td> <td> <p>GOLSOT</p> </td> </tr> </tbody> </table> <p> </p> <p><strong>Instrument information</strong></p> <table> <tbody> <tr> <td> <p>Instrument</p> </td> <td>four-circle diffractometer</td> </tr> <tr> <td> <p>Instrument type</p> </td> <td>XtaLAB Synergy Single source at home/near HyPix-Arc 100</td> </tr> <tr> <td> <p>Instrument manufacturer</p> </td> <td>Rigaku</td> </tr> <tr> <td> <p>Detector</p> </td> <td>Hybrid Pixel Array Detector</td> </tr> <tr> <td> <p>Detector type</p> </td> <td>HyPix-Arc 100</td> </tr> <tr> <td> <p>X-ray source</p> </td> <td>fine-focus sealed X-ray tube</td> </tr> <tr> <td> <p>X-ray source type</p> </td> <td>Enhance (Cu) X-ray Source</td> </tr> <tr> <td> <p>X-ray monochromator</p> </td> <td>graphite</td> </tr> </tbody> </table> <p> </p> <p><strong>Experimental information</strong></p> <table> <tbody> <tr> <td> <p>Collection probe</p> </td> <td>x-ray</td> </tr> <tr> <td> <p>Radiation type</p> </td> <td>CuK\a</td> </tr> <tr> <td> <p>Wavelength (Å)</p> </td> <td>1.54184</td> </tr> <tr> <td> <p>Collection temperature (K)</p> </td> <td>150.0(2)</td> </tr> <tr> <td> <p>Collection pressure</p> </td> <td>Sample was collected at atmospheric pressure</td> </tr> </tbody> </table> <p> </p> <p><strong>Crystal information</strong></p> <table> <tbody> <tr> <td> <p>Chemical name</p> </td> <td>1-phenyl-3,3-bis(phenylsulfanyl)prop-2-en-1-one</td> </tr> <tr> <td> <p>Chemical formula</p> </td> <td> <p>C21 H16 O S2</p> </td> </tr> <tr> <td> <p>Crystal max size (mm)</p> </td> <td> <p>0.20</p> </td> </tr> <tr> <td> <p>Crystal mid size (mm)</p> </td> <td> <p>0.11</p> </td> </tr> <tr> <td> <p>Crystal min size (mm)</p> </td> <td> <p>0.04</p> </td> </tr> <tr> <td> <p>Crystal colour</p> </td> <td> <p>yellow</p> </td> </tr> <tr> <td> <p>Crystal habit</p> </td> <td> <p>block</p> </td> </tr> <tr> <td> <p>Sample preparation</p> </td> <td> <p>Re-crystallisation from solvent: Chloroform</p> </td> </tr> </tbody> </table> <p> </p> <p><strong>Software information</strong></p> <table> <tbody> <tr> <td> <p>Software for data collection</p> </td> <td>CrysAlisPro 1.171.42.73a (Rigaku OD, 2022)</td> </tr> </tbody> </table> <p> </p> <p><strong>File information</strong></p> <p>The .par file in the folder has been modified from the original version (the unit cell is set to 10 10 10 90 90 90 to require the user to determine the unit cell when processing the data). The original .par file (along with *_peakhunt.tabbin and *_proffitpeak.tabbin files) can be found in the folder named ‘original’.</p> <table> <tbody> <tr> <td> <p>Image folders</p> </td> <td> <p>.frames/xxx.rodhypix</p> </td> </tr> <tr> <td> <p>Image format</p> </td> <td> <p>.rodhypix (Rigaku proprietary image format)</p> </td> </tr> <tr> <td> <p>Additional files</p> </td> <td> <p>CrysAlisPro input files:</p> <p>./expinfo/</p> <p>./CrysalisExpSettings.ini</p> <p>./rja230015_2.par</p> <p>./rja230015_2.run</p> <p> </p> <p>Crystal Images:</p> <p>./movie/</p> </td> </tr> </tbody> </table>
RODIN X-ray Diffraction Data 2360262
<p>This dataset is part of the Resource of Diffraction Images Newcastle (RODIN), intended for the teaching of crystallography. More information about RODIN can be found <span>on the <a title="Link to RODIN webpage on CCDC website" href="https://www.ccdc.cam.ac.uk/community/education-and-outreach/education/rodin/" target="_blank" rel="noopener">CCDC website</a></span>, as well as in the following article: </p> <p>J. Chem. Educ. 2024, 101, 10, 4276–4281 DOI: <a href="https://doi.org/10.1021/acs.jchemed.4c00797"><span>10.1021/acs.jchemed.4c00797</span></a><span> </span></p> <p>RODIN was created for educational purposes and is ideal for teaching at secondary school and University level. We also encourage its use for teaching early-stage researchers crystallographic data processing and training new diffractometer users. The diffraction images from this project can be downloaded from Zenodo and used in teaching. You can use this resource to help students understand how to go from diffraction images to a solved crystal structure. Please note that structures from these datasets are already in the Cambridge Structural Database (CSD) and you should not submit your final structure solution to the CSD or publish them, they are intended for teaching purposes only. The diffraction images are provided under a CC-BY license. </p> <p>The zip file contains X-ray diffraction images of Coumarin. A final structure solution for this data can be found in the CSD.</p> <p>The tables below summarise the data collection parameters for the experiment.</p> <p> </p> <p><strong>General information</strong></p> <table> <tbody> <tr> <td> <p>Project</p> </td> <td> <p>Resource of Diffraction Images Newcastle (RODIN)</p> </td> </tr> <tr> <td> <p>Collection Site</p> </td> <td> <p> Newcastle University, UK</p> </td> </tr> <tr> <td> <p>Sample Label</p> </td> <td>pgw240007</td> </tr> <tr> <td> <p>Linked CCDC number</p> </td> <td>2360262</td> </tr> <tr> <td> <p>CSD Refcode</p> </td> <td> <p>COUMAR23</p> </td> </tr> </tbody> </table> <p> </p> <p><strong>Instrument information</strong></p> <table> <tbody> <tr> <td> <p>Instrument</p> </td> <td>four-circle diffractometer</td> </tr> <tr> <td> <p>Instrument type</p> </td> <td>XtaLAB Synergy Single source at home/near HyPix-Arc 100</td> </tr> <tr> <td> <p>Instrument manufacturer</p> </td> <td> <p>Rigaku</p> </td> </tr> <tr> <td> <p>Detector</p> </td> <td>Hybrid Pixel Array Detector</td> </tr> <tr> <td> <p>Detector type</p> </td> <td>HyPix-Arc 100</td> </tr> <tr> <td> <p>X-ray source</p> </td> <td>fine-focus sealed X-ray tube</td> </tr> <tr> <td> <p>X-ray source type</p> </td> <td>Enhance (Cu) X-ray Source</td> </tr> <tr> <td> <p>X-ray monochromator</p> </td> <td>graphite</td> </tr> </tbody> </table> <p> </p> <p><strong>Experimental information</strong></p> <table> <tbody> <tr> <td> <p>Collection probe</p> </td> <td>x-ray</td> </tr> <tr> <td> <p>Radiation type</p> </td> <td>CuK\a</td> </tr> <tr> <td> <p>Wavelength (Å)</p> </td> <td>1.54184</td> </tr> <tr> <td> <p>Collection temperature (K)</p> </td> <td>150.0(2)</td> </tr> <tr> <td> <p>Collection pressure</p> </td> <td> <p>Sample was collected at atmospheric pressure</p> </td> </tr> </tbody> </table> <p> </p> <p><strong>Crystal information</strong></p> <table> <tbody> <tr> <td> <p>Chemical name</p> </td> <td>Coumarin</td> </tr> <tr> <td> <p>Chemical formula</p> </td> <td>C9 H6 O2</td> </tr> <tr> <td> <p>Crystal max size (mm)</p> </td> <td>0.18</td> </tr> <tr> <td> <p>Crystal mid size (mm)</p> </td> <td>0.05</td> </tr> <tr> <td> <p>Crystal min size (mm)</p> </td> <td>0.03</td> </tr> <tr> <td> <p>Crystal colour</p> </td> <td>colourless</td> </tr> <tr> <td> <p>Crystal habit</p> </td> <td>block</td> </tr> <tr> <td> <p>Sample preparation</p> </td> <td>Re-crystallisation from solvent: Diethyl Ether</td> </tr> </tbody> </table> <p> </p> <p><strong>Software information</strong></p> <table> <tbody> <tr> <td> <p>Software for data collection</p> </td> <td>CrysAlisPro 1.171.42.90a (Rigaku OD 2023)</td> </tr> </tbody> </table> <p> </p> <p><strong>File information</strong></p> <p>The .par file in the folder has been modified from the original version (the unit cell is set to 10 10 10 90 90 90 to require the user to determine the unit cell when processing the data). The original .par file (along with *_peakhunt.tabbin and *_proffitpeak.tabbin files) can be found in the folder named ‘original’.</p> <table> <tbody> <tr> <td> <p>Image folders</p> </td> <td> <p>.frames/xxx.rodhypix</p> </td> </tr> <tr> <td> <p>Image format</p> </td> <td> <p>.rodhypix (Rigaku proprietary image format)</p> </td> </tr> <tr> <td> <p>Additional files</p> </td> <td> <p>CrysAlisPro input files:</p> <p>./expinfo/</p> <p>./CrysalisExpSettings.ini</p> <p>./pgw240007.par</p> <p>./pgw240007.run</p> <p> </p> <p>Crystal Images:</p> <p>./movie/</p> </td> </tr> </tbody> </table> <p> </p>
X-ray diffraction data on the crystal structures of Tris-bound β-glucosidase from Thermoanaerobacterium saccharolyticum
<p>X-ray diffraction data of Tris-bound β-glucosidase from Thermoanaerobacterium saccharolyticum</p> <p>Data type: raw data<br>Data format: cbf</p> <p>Data <br>1. TsaBgl-Tris Data I <br>2. TsaBgl-Tris Data II<br>3. TsaBgl-Tris Data III </p>
Diffraction data for Zajdel et al Turning Molecular Springs into Nano-Shock Absorbers ACS Appl. Mater. Interfaces 2022, 14, 26699−26713
<p>Datasets required to reproduce:</p> <p>Individual files</p> <p>Fig. 1,- XRDs of materials collected on DiscoverD, CuKa</p> <p>(BT-1.zip)</p> <p>Fig. 4a. - neutron powder diffraction of ZIF-8 + 2D2O/1H2O mix collected at the BT-1 diffractometer of the NIST Center of Neutron Research at 30C. For plot the data were normalized to a common scale in counts/h</p> <p>Fig. 4c. Fullprof PCR file and VESTA model with the volmetric data *.pgrid</p> <p>Fig. 4d Single detector file Z8221010.bt1 and raw pressure output + reduced data (Zenodo_30C_drops_Fig4d.DAT).</p> <p>Fig. 4b VSANS (110) integration results Up and Down (VSANS.zip)</p>
Determination of the spinel content in cycled Li1.2Ni0.13Mn0.54Co0.13O2 using three-dimensional electron diffraction and precession electron diffraction
<p>(hkl,I)-lists for the 150 times cycled NMC material</p>
High-pressure x-ray diffraction data for claudetite II
<p>High-pressure x-ray diffraction data for claudetite II collected at the European Synchrotron Radiation Facility.</p>
High-pressure x-ray diffraction data for arsenolite and its inclusion compound with helium
<p>X-ray diffraction data for arsenolite and its inclusion compound collected at the European Synchrotron Radiation Facility.</p>
X-ray diffraction data for urotropine under high pressure - part 3 - data from ID27 beamline
<p>X-ray diffraction data for urotropine collected at the ID27 beamline of the European Synchrotron Radiation Facility under high pressure.</p>
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These curated guides explain access requirements, typical timelines, costs, and reuse considerations for widely used research datasets.
Allen Brain Atlas
Allen Brain Atlas is an Allen Institute collection of brain map atlases, datasets, APIs, and analysis tools covering mouse, human, and non-human primate brain resources.
Annotated Behaviour and Observability Dataset (ABODe)
ABODe is a University of Edinburgh DataShare dataset for behavior classification in group-housed mice using home-cage video, identities, bounding boxes, ground-plate positions, and annotator labels.
DANDI Archive for NWB datasets
DANDI is a BRAIN Initiative archive for publishing and sharing neurophysiology data, including electrophysiology, optophysiology, and behavioral data packaged as NWB and related standards.
International Brain Laboratory public data
The International Brain Laboratory public data releases expose standardized mouse decision-making experiments, including Neuropixels recordings, widefield calcium imaging, behavior, and session metadata accessed through the ONE API.
OpenNeuro
OpenNeuro is a free, open platform for sharing neuroimaging datasets, with public search, dataset pages, and download paths for web, S3, DataLad, and the OpenNeuro CLI.