{"data":{"id":"10.5281/zenodo.21114117","type":"dois","attributes":{"doi":"10.5281/zenodo.21114117","prefix":"10.5281","suffix":"zenodo.21114117","identifiers":[{"identifier":"oai:zenodo.org:21114117","identifierType":"oai"}],"alternateIdentifiers":[{"alternateIdentifierType":"oai","alternateIdentifier":"oai:zenodo.org:21114117"}],"creators":[{"name":"McGrae-Menge, Madox","nameType":"Personal","givenName":"Madox","familyName":"McGrae-Menge","nameIdentifiers":[{"nameIdentifier":"0000-0002-2779-0570","nameIdentifierScheme":"ORCID"}],"affiliation":[]}],"titles":[{"title":"Counter-streaming heat-flux closure for electron-only collisionless magnetic reconnection"}],"publisher":"Zenodo","container":{},"publicationYear":2026,"subjects":[],"contributors":[],"dates":[{"date":"2026-07-02","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsVersionOf","relatedIdentifier":"10.5281/zenodo.21114116","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"In this upload we provide the input files/data associated with the paper \"Counter-streaming heat-flux closure for electron-only collisionless magnetic reconnection\" by McGrae-Menge et al., 2026. \"input_PIC.2d\" is the OSIRIS (https://osiris-code.github.io) particle-in-cell (PIC) input deck used to create the (beta_Reconn.=0.1, B_Guide/B_Reconn.=0.1) electron-only collisionless magnetic reconnection data set used for the bulk of the first-principles analysis. The physical initialization of the simulation is described in Appendix A: PIC simulation setup. The data from this PIC simulation is located in \"BgBr0point1-Beta0point1_PIC.zip\". Since the total diagnostics are ~1.6TB we only include the moment diagnostics from t=0,300w_pe^{-1} (and raw particle data from t=300w_pe^{-1} used in Fig. 1) although the entire dataset can be created by running the attached input deck. UDIST diagnostics are defined as vfl_i=(1/n)\\int dv^3 f v_i, and v_i v_j = \\int dv^3 f v_i v_j. The parameter scan data used to create Fig. 4 is created by running the attached input deck but simply with altered B_Guide, u_th values to change B_Guide/B_{Reconn.} and beta_{Reconn.} respectively. \n\n\"input_1-e-Fluid.lua\" and \"input_2-e-Fluid.lua\" are the Gkeyll (https://gkeyll.readthedocs.io/en/latest/index.html) 10-moment 1-electron-fluid \u0026 2-electron-fluid input decks respectively used to create the (beta_Reconn.=0.1, B_Guide/B_Reconn.=0.1) electron-only collisionless magnetic reconnection fluid simulation data sets. The physical initializations of the simulations are described in Appendix C: Fluid simulation setup. We have attached the moment diagnostics from t=0,300w_pe^{-1}, located in files \"BgBr0point1-Beta0point1_1-e-Fluid.zip\" and \"BgBr0point1-Beta0point1_2-e-Fluid.zip\". Again, the full outputs can be created by running the attached input decks. We note that both simulation tools Osiris \u0026 Gkeyll are open source codes. With any questions on how to interpret the input files/simulation data please email madoxmm@physics.ucla.edu. ","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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