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33 results for “magnetic reconnection”

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zenodo48/100

Labelled magnetic reconnection simulation data set

<p>Numerical simulations have been performed on Marconi at CINECA (Italy) under the ISCRA initiative.&nbsp;The corresponding data can be found at:&nbsp;<a href="https://doi.org/10.5281/zenodo.3935887">https://doi.org/10.5281/zenodo.3935887</a></p>

opencc-by-4.0Jun 2020View details →
zenodo44/100

Reconnection rates of the paper "Simulation of plasmaspheric plume impact on dayside magnetic reconnection"

<p>This repository contains the dataset needed for the paper&nbsp;&quot;Simulation of plasmaspheric plume impact on dayside magnetic reconnection&quot;, i.e. the magnetic reconnection rates at each time and the quantities needed to normalize them. All the data are stored in the file &quot;rates_norm.h5&quot;. The file &quot;si_content.pdf&quot; explain how the data are stored and how you can extract them.</p>

opencc-by-4.0Feb 2020View details →
zenodo44/100

Three-dimensional magnetic reconnection in particle-in-cell simulations of anisotropic plasma turbulence (Simulation Data)

<p>This folder&nbsp;contains the output of the following simulation:&nbsp;</p> <p>We use the explicit Plasma Simulation Code (PSC, Germaschewski et al.2016) to simulate eight anisotropic counter-propagating Alfv&eacute;n waves in an ion-electron plasma. The anisotropy of the initial fluctuation is set up according to the theory of critical balance by Sridhar &amp; Goldreich (1994) and Goldreich &amp; Sridhar (1995) at the small scale end of the inertial range: <span class="math-tex">\(k_{\parallel} d_{i} = C (|k_{\perp}|d_{i})^{2/3}\)</span>, where <span class="math-tex">\(C= 10^{-4/3}\)</span>. The normalization parameters are the speed of light <span class="math-tex">\(c = 1\)</span>, the vacuum permittivity <span class="math-tex">\(\epsilon_{0} = 1\)</span>, the magnetic permeability <span class="math-tex">\(\mu_{0} = 1\)</span>, the Boltzmann constant <span class="math-tex">\(k_{b}=1\)</span>, the elementary charge <span class="math-tex">\(q=1\)</span>, the ion mass <span class="math-tex">\(m_{i}=1\)</span>, the density of ions and electrons <span class="math-tex">\(n_{i}=n_{e}=1\)</span>&nbsp;and the ion inertial length <span class="math-tex">\(d_{i}=c/\omega_{pi}\)</span>&nbsp;where <span class="math-tex">\(\omega_{pi}=\sqrt{n_{i}q^{2}/m_{i}\epsilon_{0}}\)</span>&nbsp;is the ion plasma frequency. We set&nbsp;<span class="math-tex">\(\beta_{s,\parallel}=1\)</span> and <span class="math-tex">\(T_{s,\parallel}/T_{s,\perp}=1\)</span>, where <span class="math-tex">\(\beta_{s,\parallel}=2 n_s \mu_{0} k_{B}T_{s,\parallel}/B_{0}^{2}\)</span>&nbsp;is the ratio between the plasma pressure parallel to the background magnetic field <span class="math-tex">\(\mathbf{B}_{0}\)</span> and the magnetic pressure and $T_{s,\parallel}$ is the parallel temperature. The magnetic field is normalised to <span class="math-tex">\(B_{0}=V_{A}/c\)</span>, &nbsp;where <span class="math-tex">\(V_{A}=B_{0} / \sqrt{\mu_{0}n_{i}m_{i}}\)</span>&nbsp;is the ion Alfv&eacute;n speed. We use 100&nbsp;particles per cell (100&nbsp;ions and 100&nbsp;electrons), a mass ratio of&nbsp;<span class="math-tex">\(m_{i}/m_{e} = 100\)</span> so that <span class="math-tex">\(d_e = 0.1 d_{i}\)</span>&nbsp;where&nbsp;<span class="math-tex">\(m_{e}\)</span> is the electron mass and <span class="math-tex">\(d_{e}\)</span>&nbsp;is the electron inertial length. The simulation box size is <span class="math-tex">\(L_{x} \times L_{y} \times L_{z} = 24d_{i}\times24d_{i}\times125d_{i}\)</span>&nbsp;and the spatial resolution is <span class="math-tex">\(\Delta x =\Delta y = \Delta z =  0.06d_{i}\)</span>. We use a time step&nbsp;<span class="math-tex">\(\Delta t =0.06/ \omega_{pi}\)</span>. In our normalisation, the Debye length <span class="math-tex">\(\lambda_{D}=d_{i}\sqrt{\beta_{i}/2}V_{A}/c\)</span> defines the minimum spatial distance that needs to be resolve in the simulation and <span class="math-tex">\(\lambda_D=0.07d_i\)</span>.</p> <p>This output corresponds to <span class="math-tex">\(t=120 \omega_{pi}\)</span>.&nbsp;</p> <p>These data were produced using the Data Intensive at Leicester (DIaL) facility&nbsp;provided by the DiRAC project<br> dp126 &quot;Identifying and Quantifying the Role of Magnetic Reconnection in Space Plasma Turbulence&quot;.</p>

opencc-by-4.0Dec 2020View details →
zenodo44/100

Data for "Impact of the Out-of-Plane Flow Shear on Magnetic Reconnection at the Flanks of Earth's Magnetopause"

<p>Data for Figures 3-8 in the paper (data for Figures 5 has been updated on 2024-09-20). The data is compatible with all data-analysis software. Here are the guidelines for reading and visualizing the data:</p> <p>(1) The filenames "noshear", "MA0p7", and "MA2p3" correspond to the simulation runs with no flow shear, Mach number M_A=0.7 flow shear, and M_A=2.3 flow shear.</p> <p>(2) The "upper" and "lower" mean upper and lower current sheet, corresponding to dusk-side and dawn-side reconnection respectively. For the "noshear" case, only the "upper" is considered.</p> <p>(3) Each data file (*.dat) is written in ASCII format and has multiple columns. The first row is the header.</p> <ul> <li>The first column is always the x-coordinates of the figure.&nbsp;</li> <li>For the line plots, all columns starting from the second column are the y-coordinates for different variables. The variables names can be found at the header.&nbsp;</li> <li>For the 2D image plots, the second column is the y-coordinates, and the third column is the value of the variable at a given (x,y) location.&nbsp;</li> </ul> <p>(4) The files "fig4_*_field_*.dat" are the magnetic potential in the x-y domain. The contour of this potential gives the in-plane field line configurations.</p>

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

Data and Software for "Determining the orientation of a magnetic reconnection X line and implications for a 2D coordinate system"

<p>Supporting information for &quot;Determining the orientation of a magnetic reconnection X line and implications for a 2D coordinate system&quot;, by Denton et al. Includes a copy of the paper and previous relevant papers, the simulation data used in the paper, and the reconstruction code used in the paper. See the readme files.</p>

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

The spreading of magnetic reconnection X-line in particle-in-cell simulations– mechanism and the effect of drift-kink instability

<p>This dataset contains data and Python scripts in "The spreading of magnetic reconnection X-line in particle-in-cell simulations&ndash; mechanism and the effect of drift-kink instability" prepared to submit to the Journal of Geophysical Research.&nbsp;</p>

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

Data files of the paper "Energy conversion by magnetic reconnection in multiple ion temperature plasmas"

<p>Reconnection rate&nbsp;and energy budget&nbsp;files for the simulations&nbsp;used in for the paper&nbsp;&quot;Energy conversion by magnetic reconnection in multiple ion temperature plasmas&quot;. The paper has two simulations. The first one, without cold ions, has his reconnection rate data stored in &quot;rate_147.dat&quot; and the&nbsp;energy budget data in &quot;Ebudget_symm_nocold_Xframe.h5&quot;. The second one,&nbsp;with&nbsp;cold ions, has his reconnection rate data stored in &quot;rate.dat&quot; and the&nbsp;energy budget data in &quot;Ebudget_symm_cold_Xframe.h5&quot;.</p> <p>On top of that is a datafile from simulation 1 at time 144.5&nbsp;(corresponding to the time of the picture A in figure 1) with all the output fields from the simulation at this given time.</p>

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

Estimates of the Wavenumber Wavelet Power Spectrum of Magnetic Fluctuations during Magnetic Reconnection Figure Data

<p>This is data for the publication, &quot;Estimates of the Wavenumber Wavelet Power Spectrum of Magnetic Fluctuations during Magnetic Reconnection&quot;.</p>

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

Dataset: 2D particle-in-cell (PIC) simulation of the magnetic reconnection for the paper "Electron mixing and isotropization in the exhaust of asymmetric magnetic reconnection with a guide field"

<p>This repository contains pubilicly available numerical data of a&nbsp;2D magnetic reconnection event, which includes&nbsp;the field data and plasma moment data. The simulation is performed with the VPIC code. The simulated data are used for the paper &quot;Electron mixing and isotropization in the exhaust of asymmetric magnetic reconnection with a guide field&quot;.&nbsp;&nbsp;</p>

opencc-by-4.0Mar 2020View details →
zenodo36/100

Intermittent Lobe Reconnection under Prolonged Northward Interplanetary Magnetic Field Condition: Insights from Cusp Spot Event Observations

<p>SuperDARN is a collection of radars funded by national scientific funding agencies of Australia, Canada, China, France, Italy, Japan, Norway, South Africa, United Kingdom and the United States of America.&nbsp;<br>We would like to thank British Antarctic Survey (https://www.bas.ac.uk/project/superdarn) and the University of Saskatchewanan (https://superdarn.ca) for hosting the SuperDARN data mirrors access.&nbsp;<br>The EISCAT dataset is available from the Madrigal database (http://millstonehill.haystack.mit.edu).&nbsp;<br>We acknowledge the use of DMSP/SSUSI data provided by the Johns Hopkins University Applied Physics Laboratory (https://cdaweb.gsfc.nasa.gov).&nbsp;<br>Additionally, the OMNI dataset is available from the OMNIWeb service online of NASA/GSFC's Space Physics Data Facility's (https://spdf.gsfc.nasa.gov/pub/data/omni/).</p>

opencc-by-4.0Dec 2023View details →
zenodo36/100

Data and Analysis Files for Simulations of Radiatively-Cooled Magnetic Reconnection on the Z machine

<p>This dataset contains processed simulation data, representative simulation output files, and Python code for analysis of simulations presented in&nbsp;Datta, Rishabh, et al. "Simulations of Radiatively Cooled Magnetic Reconnection Driven by Pulsed Power." J. Plasma Phys. (2024).</p> <p>The simulations were run using GORGON, a radiative resistive MHD code with van Leer advection.<br><br>Details on GORGON can be found in Chittenden et al. (2004) 10.1063/1.1643756, and Ciardi et al. (2007) 10.1063/1.2436479.</p>

opencc-by-4.0Mar 2024View details →
zenodo36/100

Configuration of magnetotail current sheet prior to magnetic reconnection onset

<p>Data repository for &quot;Configuration of magnetotail current sheet prior to magnetic reconnection onset&quot;. This repository contains the following files: (1) &quot;xyarray&quot; is the main dataset; (2) &quot;read_pritchett_pic_2d.py&quot; is the python module that reads xyarray; (3) &quot;simulation_params2.py&quot; is the auxiliary python module that stores simulation parameters; (3) The python scripts with prefix &quot;prod2_&quot; plot the production figures; (4) &quot;plt_style.py&quot; is the plotting style sheet; (5) &quot;movie-prod2_ratio-force.mp4&quot; shows the evolution of different terms in the momentum equation prior to magnetic reconnection (The gray lines stand for the sum of all terms).</p>

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

Data for Three-dimensional X-line spreading in asymmetric magnetic reconnection

<p>The data and IDL scripts for all the figures of our&nbsp;2019&nbsp;JGR&nbsp;are organized in a self-explanatory way.</p>

opencc-by-4.0Oct 2019View details →
zenodo32/100

Simulation data in "Intense magnetic reconnection process embedded in three-dimensional turbulent current sheet"

<p>Simulation data and program&nbsp;used for the research &quot;Intense magnetic reconnection process embedded in three-dimensional turbulent current sheet&quot;.</p>

opencc-by-4.0Nov 2023View details →
zenodo32/100

Supplemental Material for the paper "Hamiltonian model for electron heating by electromagnetic waves during magnetic reconnection with a strong guide field"

<p>Video clip showing the trajectories of two close particles in the (x,px) phase space while interacting with a wave.</p> <p>Red and green dots are the particle positions, superimposed to the instantaneous energy levels.</p>

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

Files to recreate figures in "Magnetic Reconnection on a Klein Bottle" by Xia and Swisdak (2024)

Open the record for dataset details and reuse information.

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

Kinetic Alfvén waves excited in two-dimensional magnetic reconnection

<p>Simulation data used in the paper &rdquo;Kinetic Alfv&eacute;n waves excited in two-dimensional magnetic reconnection&quot;, submitted to JGR-Space Physics.</p> <p>The directory contains the input file, output data and post-processing script from running iPIC3D for investigating the kinetic Alfv&eacute;n waves in magnetic reconnection, while the code iPIC3D is available on <a href="https://bitbucket.org/bopkth/ipic3d-klm">https://bitbucket.org/bopkth/ipic3d-klm</a>.</p> <p>Each case represents different thickness of the current sheet. The details are described in the paper.</p>

opencc-by-sa-4.0Apr 2018View details →
zenodo32/100

Example Data for the MARZ Magnetic Reconnection Experiments

<p>This dataset contains example data used in the MARZ magnetic reconnection expeirments.</p> <p>Experimental details are in:</p> <p>[1] R. Datta et al. (2024) PRL.&nbsp;<a href="https://doi.org/10.1103/physrevlett.132.155102" rel="nofollow">https://doi.org/10.1103/physrevlett.132.155102</a>&nbsp;<br>[2] R. Datta, et al. (2024). Phys. Plasmas.&nbsp;<a href="https://doi.org/10.1063/5.0201683" rel="nofollow">https://doi.org/10.1063/5.0201683</a></p> <p>Analysis code can be downloaded from <a href="https://github.com/ridatta/MARZ_Analysis_Tools.git">https://github.com/ridatta/MARZ_Analysis_Tools.git&nbsp;</a></p> <p>Diagnostics details are in Webb, Timothy Jay, et al. Review of Scientific Instruments 94.3 (2023).&nbsp;<a href="https://doi.org/10.1063/5.0123448" rel="nofollow">https://doi.org/10.1063/5.0123448</a></p> <p>The diagnostics in MARZ include:</p> <p>(1) B-Dots/ Inductive Probes.</p> <p>Data from each probe is stored as .CSV files.&nbsp;</p> <p>(2) Visible Spectroscopy (SVS)</p> <p>Data is stored in HDF files. For pre-processing, we need shot data, as well as calibration data, which includes pre-shot laser images, LDLS fast and slow images, and Tungsten lamp images.&nbsp;</p> <p>(3) XRS3 (X Ray Spectroscopy)</p> <p>Data is stored in TIFF files.&nbsp;</p> <p>(4) Ultra-Fast X Ray Pinhole Cameras</p> <p>Data is stored in TIFF files.&nbsp;</p> <p>(5) Self Emission Gated Optical Imager (SEGOI)</p> <p>SEGOI outputs 2D time-resolved optical emission data, and 1-D space- and time-resolved streak image data, stored in HDF5 format.</p> <p>(6) X Ray Diodes (TADPoles and LOS 170 Silicon Diodes)</p> <p>Data is stored in CSV files.&nbsp;</p>

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

Simulation dataset for Off-diagonal Ion Pressure Linked to Hall Fields in Collisionless Magnetic Reconnection

<p>The dataset contains simulation data used in the paper of "Off-diagonal Ion Pressure LInked to Hall Fields in Collisionless Magnetic Reconnection". Data are generated from a particle-in-cell simulation using the VPIC code. Please see the paper for the descriptions of the simulation setup.</p> <p>The .gda files in fiels_moments_gda_files.zip are fields and plasma moments data from the time step presented in the paper. Each file contains float-type data arrays with a size of 6720x1x2240, corresponding to x-y-z dimensions, respectively. Data can be read by softwares like IDL, python, matlab, etc., using the standard data reading methods.</p> <p>The file of harris_m100_x60_Hparticle.89586 contains ion particle data for this time step, for the domain of x=[0,60]di, z=[-8,8]di. The file is written in BINARY, for the information of indivial particles. Each data chunk constitues of the following variables in order: x, z, ux, uy, uz, q. Here x and z are positions of the particles, in unit of de; ux, uy, uz are relativistic velocities in unit of the speed of light (c), i.e., ux = gamma*vx, gamma=sqrt(1+ux^2+uy^2+uz^2); q represents the weight of the particles, so the contribution of a particle to the phase space density needs to multiply by this q factor (In the paper, q factors are re-normalized while the relative weights between particles remain the same).</p> <p>An example IDL sentence of reading particle data: readu, lun, x, z, ux, uy, uz, q. Repeat this sentence for different particles.</p>

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

Dataset for "Identifying The Growth Phase of Magnetic Reconnection using Pressure-Strain Interaction"

<p>Simulation dataset for the "Identifying The Growth Phase of Magnetic Reconnection using Pressure-Strain Interaction"</p>

opencc-by-4.0Sep 2024View details →

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