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21 results for “AGB”

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zenodo48/100

Aboveground Biomass (AGB) measurements at Hartheim Forest Research Site (DE-Har) 2023

<p>Aboveground biomass (AGB) estimated at the&nbsp;<a href="https://www.meteo.uni-freiburg.de/en/infrastructure/hartheim-forest-research-site">Hartheim Forest Research Site</a> (ICOS Ecosystem Site &ldquo;DE-Har&rdquo;) in Fall 2023 gathered in compliance with ICOS instructions for AGB determination.</p> <p>Associated Ecoystem Site in the Integrated Carbon Observation System (ICOS).</p> <p>Site Metadata:</p> <p>Station Name: Hartheim-DE-HAR<br>Station ID: DE-Har<br>Station Address: Hartheim am Rhein, Germany<br>Station Longitude: 7.59814 deg E<br>Station Latitude: 47.93391 deg N<br>Station Elevation: 201 m</p>

opencc-by-4.0Mar 2024View details →
zenodo44/100

Three-component modelling of O-rich AGB star winds I. Effects of drift using forsterite – dataset

<p>The data provided here include all parameter files, log files, and a set of the<br> binary output files that are the basis for the publication in A&amp;A.</p> <p>The file &#39;file_listing.txt&#39; contains a complete list of files and directories<br> in all gzipped tar files. Each individual gzipped tar file is formatted as<br> follows:</p> <p>&nbsp;Mm.m_Ll.ll_Ttttt.tar.gz</p> <p>where<br> &nbsp;m.m&nbsp; :: the assumed mass of the model, in solar masses<br> &nbsp;l.ll :: The assumed luminosity, in log10(solar luminosities)<br> &nbsp;tttt :: The effective temperature of the star, in Kelvin.</p> <p><br> The contents of the tar files vary according to the model, but here is the<br> general directory structure:</p> <p>&nbsp;nodr/&nbsp; :: non-drift / PC models<br> &nbsp;drift/ :: drift models</p> <p>&nbsp;nodr/init<br> &nbsp;drift/init :: Initial model files created using John Connor.</p> <p><br> File suffixes are the following:</p> <p>&nbsp;.par :: Plain-text parameter file that contains all parameters that are<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; different from the respective default value in the model.<br> &nbsp;&nbsp; &nbsp; Consequently, to see what parameters were actually used, it is<br> &nbsp;&nbsp; &nbsp; necessary to look in the log file (see below).</p> <p>&nbsp;.bin :: Binary file that contains output of converged models. Each model is<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; stored in two versions, first the previous time step and then the<br> &nbsp;&nbsp; &nbsp; current time step (having access to the model code T-800, data of both<br> &nbsp;&nbsp; &nbsp; time steps are needed to restart model calculations at that time<br> &nbsp;&nbsp; &nbsp; step).</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; The initial model file only contains one model; where the previous<br> &nbsp;&nbsp; &nbsp; time step data are the same as the current time step data.</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; We provide a tool to read this file, see below.</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Note! These files can get pretty large and are therefore only<br> &nbsp;&nbsp; &nbsp;&nbsp;&nbsp; available for a smaller number of the models in the Zenodo dataset.<br> &nbsp;&nbsp; &nbsp;&nbsp;&nbsp; Please ask the corresponding author for the missing files is the<br> &nbsp;&nbsp; &nbsp;&nbsp;&nbsp; need should appear.</p> <p>&nbsp;.log :: Plain-text log file that shows the used model parameters and a number<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; of key properties for each converged model.<br> &nbsp;&nbsp; &nbsp; The encoding of this file is UTF-8.</p> <p>&nbsp;.inf :: Plain-text secondary log file that contains the header of the<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; [primary] log file as well as timing information.<br> &nbsp;&nbsp; &nbsp; The encoding of this file is UTF-8.</p> <p>&nbsp;.tpb :: Secondary binary file that contains a number of properties specified<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; at the outer boundary, typically for each consecutive time step.</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; We provide a tool to read this file, see below.</p> <p>&nbsp;.lis :: Plain-text file with the iteration history. Unavailable here.</p> <p>&nbsp;.liv :: Plain-text file with values specified for a number of properties at<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; each gridpoint. Unavailable here.</p> <p>&nbsp;.inp :: Plain-text file that is used to launch a model; some are present.<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; This file is automatically generated by the tool that launches T-800<br> &nbsp;&nbsp; &nbsp; and is typically removed when T-800 launches. Unavailable here.</p> <p>&nbsp;.eps :: Encapsulated PostScript file created by John Connor when calculating<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; the initial model.</p> <p><br> Model evolution structure - file endings before the suffix:</p> <p>&nbsp;_rlx :: Files related to relaxing the T-800 calculations on the initial model<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; created by John Connor.</p> <p>&nbsp;_exp :: Files related to expanding the initially compact model to using the<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; full radial domain.</p> <p>&nbsp;_fix :: Files related to the intermediate stage where calculations are changed<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; from expansion to outflow.<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; &nbsp;<br> &nbsp;_out :: Files related to the outflow stage of the calculations; this is what<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; you want to look at to see the wind evolution. Results in the paper<br> &nbsp;&nbsp; &nbsp; are calculated using these data.</p> <p>&nbsp;Note! Some outflow stage calculations continue the evolution of the previous<br> &nbsp;&nbsp; set of files. The underlying reason for continued calculations is typically<br> &nbsp;&nbsp; that the calculated time interval is too short. Such files are typically<br> &nbsp;&nbsp; given the extension &#39;_cont.lin_out&#39;, &#39;_cont2.lin_out&#39;, etc.</p> <p><br> Stored data in the binary files:</p> <p>&nbsp;The binary files (suffix &#39;.bin&#39;) contain the full radial structure in the<br> &nbsp;following 10 (PC models) or 11 (drift models) primary variables:</p> <p>&nbsp;&nbsp; mr: radius<br> &nbsp;&nbsp; mm: integrated [gas] mass<br> &nbsp;&nbsp; md: gas density<br> &nbsp;&nbsp; mu: gas velocity<br> &nbsp;&nbsp; me: internal energy<br> &nbsp;&nbsp; mj: radiative energy<br> &nbsp;&nbsp; mh: radiative flux<br> &nbsp;&nbsp; n0: dust moment, forsterite (Fo)<br> &nbsp;&nbsp; nm: number density of magnesium atoms<br> &nbsp;&nbsp; ns: number density of silicon atoms<br> &nbsp;&nbsp; v0: dust velocity, forsterite (only drift models)</p> <p>&nbsp;Other properties are derived from these primary variables using auxiliary code<br> &nbsp;that isn&#39;t part of this dataset.</p> <p><br> Load files:</p> <p>&nbsp; Two tools are provided here that can load the binary data files using the<br> &nbsp; Interactive Data Language (IDL):</p> <p>&nbsp; sc_load_bin (for files with the suffix &#39;.bin&#39;):</p> <p>&nbsp;&nbsp;&nbsp; Loads the full content of a T-800 binary file and returns a structure<br> &nbsp;&nbsp;&nbsp; with the data.</p> <p><br> &nbsp; sc_load_tpb (for files with the suffix &#39;.tpb&#39;):</p> <p>&nbsp;&nbsp;&nbsp; Loads the full content of a T-800 &#39;tpb&#39; binary file and returns a<br> &nbsp;&nbsp;&nbsp; structure with the data.</p> <p>&nbsp;&nbsp;&nbsp; Note! Due to the way models run on clusters, this file is sometimes<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; incomplete; this happens when the model code T-800 is stopped as the<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; cluster-specific walltime is reached. If this is the case, it is<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; necessary to use the binary file instead, where data are saved<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; typically every 20:th time step.</p> <p>&nbsp; Alternative tools for use with Python and Julia could be considered for<br> &nbsp; writing, but where not yet available when this dataset was made public.<br> &nbsp; Please contact the corresponding author for a current status on this issue.</p> <p>&nbsp;</p>

opencc-by-4.0Jun 2023View details →
zenodo40/100

Three-component modelling of C-rich AGB-star winds V. – dataset

<p>The provided data include all parameter files, binary output files, and log<br> files that are the basis for the publication in MNRAS.</p> <p>The file &#39;file_listing.txt&#39; contains a complete list of files and<br> directories in all gzipped tar files. Each individual gzipped tar file is<br> formatted as follows:</p> <p>&nbsp;Mm.m_Ll.ll_Ttttt_CtOc.cc.tar.gz</p> <p>where<br> &nbsp;m.m&nbsp; :: the assumed mass of the model, in solar masses<br> &nbsp;l.ll :: The assumed luminosity, in log10(solar luminosities)<br> &nbsp;tttt :: The effective temperature of the star, in Kelvin.<br> &nbsp;c.cc :: The carbon-to-oxygen excess, in log10(n_C/n_H-n_O/n_H)+12</p> <p><br> The contents vary according to the model, but here is the general directory<br> structure:</p> <p>&nbsp;nodr/&nbsp; :: non-drift / PC models<br> &nbsp;drift/ :: drift models</p> <p>&nbsp;nodr/init<br> &nbsp;drift/init :: Initial model files created using John Connor.</p> <p><br> File suffixes are the following:</p> <p>&nbsp;.par :: Plain-text parameter file that contains all parameters that are<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; different from the respective default value in the model.<br> &nbsp;&nbsp; &nbsp; Consequently, to see all used parameters it is necessary to look in<br> &nbsp;&nbsp; &nbsp; the log file (see below).</p> <p>&nbsp;.bin :: Binary file that contains converged models. Each model is stored in<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; two versions, first the previous time step and then the current time<br> &nbsp;&nbsp; &nbsp; step (both are needed to restart model calculations at that time<br> &nbsp;&nbsp; &nbsp; step).</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; The initial model file only contains one model; where the previous<br> &nbsp;&nbsp; &nbsp; time step data are the same as the current time step data.</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; The format of this file is explained below.</p> <p>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Note! These files can get pretty large and are therefore only<br> &nbsp;&nbsp; &nbsp;&nbsp;&nbsp; available for a smaller number of the models here. Please ask the<br> &nbsp;&nbsp; &nbsp;&nbsp;&nbsp; corresponding author for the missing files should the need appear.</p> <p>&nbsp;.log :: Plain-text log file that shows the used model parameters and a number<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; of key properties for each converged model. The encoding of this file<br> &nbsp;&nbsp; &nbsp; is UTF-8.</p> <p>&nbsp;.inf :: Plain-text secondary log file that contains the header of the<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; [primary] log file as well as timing information.</p> <p>&nbsp;.tpb :: Secondary binary file that contains a number of properties specified<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; at the outer boundary, typically for each consecutive time step.</p> <p>&nbsp;.lis :: Plain-text file with the iteration history. Available for some files.</p> <p>&nbsp;.liv :: Plain-text file with values specified for a number of properties at<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; each gridpoint. Available for a smaller number of files.</p> <p>&nbsp;.inp :: Plain-text file that is used to launch a model; some are still there.</p> <p>&nbsp;.eps :: Encapsulated PostScript files created by John Connor when calculating<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; the initial model.</p> <p><br> Model evolution structure - file endings before the suffix:</p> <p>&nbsp;_rlx :: Files related to relaxing the T-800 calculations on the initial model<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; created by John Connor.</p> <p>&nbsp;_exp :: Files related to expanding the initially compact model to using the<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; full radial domain.</p> <p>&nbsp;_fix :: Files related to the intermediate stage where calculations are changed<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; from expansion to outflow.<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; &nbsp;<br> &nbsp;_out :: Files related to the outflow stage of the calculations; this is what<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; you want to look at to see the wind evolution. Results in the paper<br> &nbsp;&nbsp; &nbsp; are calculated using these data.</p> <p>&nbsp;<br> &nbsp;Note! Some outflow stage calculations continue the evolution of the previous<br> &nbsp;&nbsp; set of files. The underlying reason for continued calculations is typically<br> &nbsp;&nbsp; that the calculated time interval is too short. Such files are typically<br> &nbsp;&nbsp; given the extension &#39;_cont.lin_out&#39;, &#39;_cont2.lin_out&#39;, etc.</p> <p><br> Load files:</p> <p>&nbsp; Two tools are provided here that can load the binary data files using the<br> &nbsp; Interactive Data Language (IDL):</p> <p>&nbsp; sc_load_bin (for files with the suffix &#39;.bin&#39;):</p> <p>&nbsp;&nbsp;&nbsp; Loads the full content of a T-800 binary file and returns a structure<br> &nbsp;&nbsp;&nbsp; with the data.</p> <p><br> &nbsp; sc_load_tpb (for files with the suffix &#39;.tpb&#39;):</p> <p>&nbsp;&nbsp;&nbsp; Loads the full content of a T-800 &#39;tpb&#39; binary file and returns a<br> &nbsp;&nbsp;&nbsp; structure with the data.</p> <p>&nbsp;&nbsp;&nbsp; Note! Due to the way models run on clusters, this file is sometimes<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; incomplete; this happens when the model code T-800 is stopped as the<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; cluster-specific walltime is reached. If this is the case, it is<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; necessary to use the binary file instead, where data are saved<br> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp; typically every 20:th time step.</p> <p>&nbsp; Alternative tools for use with Python and Julia could be considered for<br> &nbsp; writing, but where not yet available when this dataset was made public.<br> &nbsp; Please contact the corresponding author for a current status on this issue.</p>

opencc-by-4.0Oct 2020View details →
zenodo40/100

Aboveground Biomass (AGB) in the Boreal Region: Dataset for Supporting Biomass Recovery Analysis

<p>This package supplements the following paper submitted to Nature: <strong>Biomass recovery carbon gains surpass fire losses over boreal forests during the last decades</strong>.<br>This dataset contains the Aboveground Biomass (AGB) map (unit: Mg/ha) for the&nbsp;boreal region in 2020 at ~100m resolution.</p><p>The global AGB dataset, upon which this regional subset is based, was initially developed by Yu et al. (2023). The preprint&nbsp;version of the corresponding AGB data paper has been made available online and can be accessed at <a href="https://doi.org/10.5281/zenodo.7583611">https://doi.org/10.5281/zenodo.7583611</a>. This paper is currently under peer review. The AGB map for the boreal region, as featured in our Nature submission, is provided here for reference and further research.</p><p>&nbsp;</p><p>&nbsp;</p>

opencc-by-4.0Dec 2023View details →
zenodo40/100

AGB_VM: 0.25-degree gridded annual aboveground biomass estimates in Alaska and northwestern Canada 2003-2017..

<p>Gridded 0.25-degree annual estimates of aboveground vegetation biomass (AGB) for diverse arctic and boreal ecosystems in Alaska and northwestern Canada years 2003-2017. AGB was estimated from integrated microwave vegetation optical depth (VOD) (Vegetation Optical Depth Climate Archive (VODCA) (Moesinger et al., 2020)) and optical-multispectral vegetation indices from the MODerate Resolution Imaging Spectroradiometer (MODIS) satellite remote sensing datasets. This work was conducted through NASA's Arctic and Boreal Vulnerability Experiment (ABoVE).&nbsp;</p>

opencc-by-4.0Mar 2024View details →
zenodo40/100

Cool, Luminous, and Highly Variable Stars in the Magellanic Clouds. II: Spectroscopic Data of Thorne-Zytkow Object and Super-AGB Star Candidates

<p>This dataset contains Magellan MIKE spectroscopy of a population of cool, luminous stars in the Magellanic Clouds, a sample of confirmed Magellanic Cloud red supergiants, and spectrophotometric standard stars. The spectra were analyzed in the paper &quot;Cool, Luminous, and Highly Variable Stars in the Magellanic Clouds. II: Spectroscopic and Environmental Analysis of Thorne-\.Zytkow Object and Super-AGB Star Candidates&quot; by O&#39;Grady et al. (2022). More details are provided in the README.&nbsp;</p>

opencc-by-4.0Nov 2022View details →
zenodo36/100

A WISE view of extreme AGB stars

<p>The files in this distribution are related to the paper:</p> <p>&quot;A WISE view of extreme AGB stars&quot;, by M.A.T. Groenewegen&nbsp; published in Astronomy &amp; Astrophysics 659, A145 (2022).<br> &nbsp;</p>

opencc-by-4.0Dec 2021View details →
zenodo36/100

The C-flame Quenching by Convective Boundary Mixing in Super-AGB Stars and the Formation of Hybrid C/O/Ne White Dwarfs and SN Progenitors

<p>MESA inlists associated with <a href="https://ui.adsabs.harvard.edu/#abs/2013ApJ...772...37D/abstract">Denissenkov et al. (2013)</a>. MESA version 4631.</p> <p>Publication DOI:&nbsp;<a href="https://doi.org/10.1088/0004-637X/772/1/37">10.1088/0004-637X/772/1/37</a></p>

opencc-by-4.0Mar 2019View details →
zenodo36/100

Dust formation and mass loss around intermediate-mass AGB stars with initial metallicity Zini ≤ 10-4 in the early Universe - I. Effect of surface opacity on stellar evolution and the dust-driven wind

<p>MESA inlists associated with&nbsp;<a href="https://ui.adsabs.harvard.edu/?#abs/2017MNRAS.466.1709T">Dust formation and mass loss around intermediate-mass AGB stars with initial metallicity Zini&nbsp;&le; 10-4&nbsp;in the early Universe - I. Effect of surface opacity on stellar evolution and the dust-driven wind</a></p>

opencc-by-4.0Mar 2019View details →
zenodo36/100

SPH modelling of companion-perturbed AGB outflows including a new morphology classification scheme

<p><strong>ABSTRACT</strong></p> <p><em>Context.</em> Asymptotic giant branch (AGB) stars are known to lose a significant amount of mass by a stellar wind, which controls the remainder of their stellar lifetime. High angular-resolution observations show that the winds of these cool stars typically exhibit mid- to small-scale density perturbations such as spirals and arcs, believed to be caused by the gravitational interaction with a (sub-)stellar companion.<br> <em>Aims.</em> We aim to explore the effects of the wind-companion interaction on the 3D density and velocity distribution of the wind, as a function of three key parameters: wind velocity, binary separation and companion mass. For the first time, we compare the impact on the outflow of a planetary companion to that of a stellar companion. We intend to devise a morphology classification scheme based on a singular parameter.<br> <em>Methods.</em> We ran a small grid of high-resolution polytropic models with the smoothed particle hydrodynamics (SPH) numerical code Phantom to examine the 3D density structure of the AGB outflow in the orbital and meridional plane and around the poles. By constructing a basic toy model of the gravitational acceleration due to the companion, we analysed the terminal velocity reached by the outflow in the simulations.<br> <em>Results.</em> We find that models with a stellar companion, large binary separation and high wind speed obtain a wind morphology in the orbital plane consisting of a single spiral structure, of which the two edges diverge due to a velocity dispersion caused by the gravitational slingshot mechanism. In the meridional plane the spiral manifests itself as concentric arcs, reaching all latitudes. When lowering the wind velocity and/or the binary separation, the morphology becomes more complex: in the orbital plane a double spiral arises, which is irregular for the closest systems, and the wind material gets focussed towards the orbital plane, with the formation of an equatorial density enhancement (EDE) as a consequence. Lowering the companion mass from a stellar to a planetary mass, reduces<br> the formation of density perturbations significantly.<br> <em>Conclusions.</em> With this grid of models we cover the prominent morphology changes in a companion-perturbed AGB outflow: slow winds with a close, massive binary companion show a more complex morphology. Additionally, we prove that massive planets are able to significantly impact the density structure of an AGB wind. We find that the interaction with a companion affects the terminal velocity of the wind, which can be explained by the gravitational slingshot mechanism. We distinguish between two types of wind focussing to the orbital plane resulting from distinct mechanisms: global flattening of the outflow as a result of the AGB star&rsquo;s orbital motion and the formation of an EDE as a consequence of the companion&rsquo;s gravitational pull. We investigate different morphology classification schemes and uncover that the ratio of the gravitational potential energy density of the companion to the kinetic energy density of the AGB outflow yields a robust classification parameter for the models presented in this paper.</p>

opencc-by-4.0Jun 2021View details →
zenodo32/100

The VMC Survey - XXXVII. Pulsation periods of dust enshrouded AGB stars in the Magellanic Clouds

<p>FigA1.tar and FigC2.tar contain postscript files of the 1299 light curves&nbsp; and 254 spectral energy distributions, respectively, as described in the paper.</p>

opencc-by-4.0Mar 2020View details →
zenodo32/100

AGB_China's boreal forests_10m_2018

Open the record for dataset details and reuse information.

opencc-by-4.0Jun 2024View details →
zenodo32/100

Data for "SPH modelling of AGB wind morphology in hierarchical triple systems & comparison to observation of R Aql"

<div> <p>Additional material to Malfait et al. 2024, subm. "SPH modelling of AGB wind morphology in hierarchical triple systems &amp; comparison to observation of R Aql"</p> <p>This contains input files and final output dumps of the Phantom simulations of this paper.</p> <p>The code used to perform the simulations is available at:&nbsp;<a href="https://github.com/danieljprice/phantom">https://github.com/danieljprice/phantom.</a></p> <p>Splash (<a href="https://github.com/danieljprice/splash">https://github.com/danieljprice/splash</a>&nbsp;) and Plons (<a href="https://github.com/Ensor-code/plons">https://github.com/Ensor-code/plons</a>&nbsp;) were used to create figures and plots from this data.</p> <p>&nbsp;</p> </div>

opencc-by-4.0Jul 2024View details →
zenodo32/100

Appendices A-B-C for Malfait et al. 2024(a), Impact of HI cooling and study of accretion disks in AGB wind-companion smoothed particle hydrodynamic simulations

<p>Appendices A, B, C with figures, of the paper Malfait et al. 2024(a) "Impact of HI cooling and study of accretion disks in AGB wind-companion smoothed particle hydrodynamic simulations".</p>

opencc-by-4.0Sep 2024View details →
zenodo32/100

Correlations between the abundances of Barium stars, the AGB model residuals and the delta parameter

<p>Additional figures for Vil&aacute;gos et al. 2024, Sect. 3.2. For the sample of Barium stars, correlations between the observationally dervied abundances; the residuals between the AGB models and the abundances; and the delta parameter.</p> <p>The figures are divided into the following directories:</p> <ul> <li>'1-obs_feh':&nbsp; Abundances and elemental ratios of different peaks as a function of the [Fe/H] (Sect. 3.2.1 and Fig. 5).</li> <li>'2-res_feh':&nbsp;&nbsp; Residuals of the abundances and elemental ratios as a function of the [Fe/H] (Sect. 3.2.2 and Fig. 6).</li> <li>'3-obs_obs': Abundances as a function of the other abundances (Sect. 3.2.3 and Fig. 7).</li> <li>'4-res_res':&nbsp;&nbsp; Residuals of the abundances as a function of the other residuals (Sect. 3.2.4 and Fig. 8).</li> <li>'5-res_obs':&nbsp; Residuals of the abundances as a function of the abundances (see Sect. 3.2.5 and Fig. 9).</li> <li>'6-delta':&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Abundances and residuals as a function of the delta parameter, that indicates the fraction of AGB material in the Ba star envelope (Sect. 3.2.6 and Fig. 10).</li> </ul> <p>For figures in directories 1-2, we refer to some elements as [A/B], although sometimes [B/A] vs. [Fe/H] is shown. Visually, this swapping of the numerator and denominator elements means a vertical reflection around the y = 0 axis. Thus, $r_S$ and $a$ for [B/A] vs. [Fe/H] have the same absolute value but different sign than for [A/B] vs. [Fe/H].</p> <p>For figures in directories 3-5, if we refer to [A/Fe] vs [B/Fe], but plot [B/Fe] vs [A/Fe], the sign of the relationship (correlation or anti-correlation) remains the same. The swap of the two axes results in a reflection around a diagonal line with a slope of 1. The resulting slope is therefore $1/a$, while $r_S$ is the same in both cases.</p>

opencc-by-4.0May 2024View details →
zenodo28/100

DEATHSTAR - Nearby AGB stars with the Atacama Compact Array

<p>Low- and intermediate-mass stars develop slow and massive stellar winds when they reach the end of their lives. Investigating the mass-loss phenomenon on the asymptotic giant branch (AGB) is crucial in gaining a better understanding of late stellar evolution, as well as of the galactic chemical evolution, as AGB stars contribute significantly to the enrichment of the interstellar medium. &nbsp;DEATHSTAR is a large project aimed at improving the accuracy of stellar wind-parameter measurements. Constraining the size of the CO-emitting circumstellar envelope is the first step of the project, by mapping the envelopes &nbsp;in&nbsp; CO J=2&ndash;1 and 3&ndash;2 lines with the Atacama Compact Array (ACA). The first published DEATHSTAR sample consists of 69 nearby (&lt;1 kpc) AGB stars of the three chemical types. In this video, I present the results from our initial analysis and the current status of the DEATHSTAR project.</p>

opencc-by-4.0Dec 2021View details →
dryad28/100

Regeneration biomass (AGB & BGB), age, NSCs and light: F. sylvatica and Acer spp.

<p><span>Being able to persist in deep shade is an important characteristic of juvenile trees often leading to a strong dominance of shade-tolerant species in forests with low canopy turnover and disturbance rate. While leaf, growth and storage traits are known to be key components of shade tolerance, their interplay during regeneration development and influence on juveniles' survival time remains unclear. We assessed the ontogenetic effects of these three traits on survival time of beech  (Fagus sylvatica), Norway and sycamore maples (Acer pseudoplatanus, Acer platanoides) in a primeval beech forest. Biomass allocation, age and content of non-structural carbohydrates (NSC) were measured in stems and roots of 289 seedlings and saplings in high and low vitality classes. Saplings experience a trade-off between absolute growth rate (AGR), and storage (NSC) at decreasing leaf area ratio (LAR) with biomass development. High LAR but slow AGR and low NSC confer beech with a marked ability to persist in deep shade awaiting canopy release. In turn, a comparably small LAR in combination with fast AGR and higher storage (NSC), as observed in Norway maple and sycamore maple, reduces their survival time, thus offering an explanation for beech dominance and maples disappearance in the undergrowth of old-growth beech forests.</span></p>

opencc-zeroJun 2022View details →
zenodo28/100

Supplementary material for "Millimetre observations of the S-type AGB star χ Cygni: variability of the emission of the inner envelope"

Open the record for dataset details and reuse information.

opencc-by-4.0Sep 2024View details →
zenodo28/100

Data for 'SPH modelling of wind-companion interactions in eccentric AGB binary systems'

<p>Additional material to "Malfait et al. 2021, SPH modelling of wind-companion interactions in eccentric AGB binary systems": &nbsp;<a href="https://ui.adsabs.harvard.edu/link_gateway/2021A&amp;A...652A..51M/arxiv:2107.01074" target="_blank" rel="noreferrer noopener">arXiv:2107.01074</a></p> <p>This contains input files and final output dumps of the Phantom simulations of this paper, and additional movies of 4 of the simulations.</p> <p>The code used to perform the simulations is available at: <a href="https://github.com/danieljprice/phantom">https://github.com/danieljprice/phantom.</a></p> <p>Splash (<a href="https://github.com/danieljprice/splash">https://github.com/danieljprice/splash</a> ) and Plons (<a href="https://github.com/Ensor-code/plons">https://github.com/Ensor-code/plons</a> ) were used to create figures and plots from this data.</p>

opencc-by-4.0Jul 2021View details →
dryad28/100

Regeneration biomass (AGB & BGB), age, NSCs and light: F. sylvatica and Acer spp.

Open the record for dataset details and reuse information.

publicJun 2022View details →

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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.

allen-brain-atlas
neuroscienceopenDocumentation, web resources, and API references are available online.
Last verified 2026-04-30Open record

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.

abode-home-cage
behavioral-neuroscienceopenThe DataShare record exposes download links for annotations, documentation, license text, and the zipped per-snippet data directory.
Last verified 2026-04-30Open record

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.

dandi-nwb
electrophysiologyopenPublished Dandiset metadata and archive endpoints are available through the production DANDI API.
Last verified 2026-04-30Open record

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.

ibl
behavioral-neuroscienceopenPublic sessions can be searched and loaded from the IBL public data server through ONE.
Last verified 2026-04-29Open record

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.

openneuro
neuroscienceopenPublished datasets are available on demand over the internet.
Last verified 2026-04-29Open record