{"id":3230995,"identifier":"DVN/X6XQTM","persistentUrl":"https://doi.org/10.7910/DVN/X6XQTM","protocol":"doi","authority":"10.7910","separator":"/","publisher":"Harvard Dataverse","publicationDate":"2018-09-25","storageIdentifier":"file://10.7910/DVN/X6XQTM","datasetType":"dataset","datasetVersion":{"id":143758,"datasetId":3230995,"datasetPersistentId":"doi:10.7910/DVN/X6XQTM","storageIdentifier":"file://10.7910/DVN/X6XQTM","versionNumber":1,"versionMinorNumber":0,"versionState":"RELEASED","latestVersionPublishingState":"RELEASED","deaccessionLink":"","UNF":"UNF:6:VCd4fG0yqyI1tXZGUsdMYA==","lastUpdateTime":"2018-09-25T15:55:15Z","releaseTime":"2018-09-25T15:55:15Z","createTime":"2018-09-25T15:54:06Z","publicationDate":"2018-09-25","citationDate":"2018-09-25","termsOfUse":"This dataset is made available without information on how it can be used. You should communicate with the Contact(s) specified before use.","fileAccessRequest":false,"metadataBlocks":{"citation":{"displayName":"Citation Metadata","name":"citation","fields":[{"typeName":"title","multiple":false,"typeClass":"primitive","value":"The mechanism of plasma electron hole transverse instability"},{"typeName":"author","multiple":true,"typeClass":"compound","value":[{"authorName":{"typeName":"authorName","multiple":false,"typeClass":"primitive","value":"I. H. Hutchinson"}}]},{"typeName":"datasetContact","multiple":true,"typeClass":"compound","value":[{"datasetContactEmail":{"typeName":"datasetContactEmail","multiple":false,"typeClass":"primitive","value":"hutch@psfc.mit.edu"}}]},{"typeName":"dsDescription","multiple":true,"typeClass":"compound","value":[{"dsDescriptionValue":{"typeName":"dsDescriptionValue","multiple":false,"typeClass":"primitive","value":"It is shown through multidimensional particle-in-cell simulation that the transverse instability of plasma electron holes is caused   not by the previously proposed focusing of trapped particles, but   instead by kinematic jetting of marginally passing electrons. The   mechanism is explained and heuristic analytic estimates obtained   which agree with the growth rates and transverse wave-numbers   observed in the simulations."}}]},{"typeName":"subject","multiple":true,"typeClass":"controlledVocabulary","value":["Physics"]},{"typeName":"keyword","multiple":true,"typeClass":"compound","value":[{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"holes"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"instability"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"nonlinear theory"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"PIC"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"space plasmas"}}]},{"typeName":"notesText","multiple":false,"typeClass":"primitive","value":"<a href=\"http://library.psfc.mit.edu/catalog/reports/2010/18ja/18ja003/abstract.php\">PSFC REPORT PSFC/JA-18-3</a><br /><br />This work was partially supported by NASA grant NNX16AG82G. Computer simulations were carried out on the MIT PSFC parallel AMD Opteron/Infiniband cluster Loki, and on the MIT-PSFC partition of the Engaging cluster at the MGHPCC facility (www.mghpcc.org) which was funded by DoE grant number DE-FG02-91-ER54109."}]}},"files":[{"description":"","label":"18ja003_archival_manuscript.pdf","restricted":false,"version":1,"datasetVersionId":143758,"dataFile":{"id":3230996,"persistentId":"doi:10.7910/DVN/X6XQTM/RXSDU0","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/RXSDU0","filename":"18ja003_archival_manuscript.pdf","contentType":"application/pdf","friendlyType":"Adobe PDF","filesize":461737,"description":"","storageIdentifier":"s3://dvn-cloud:166124bcca3-ff4d69ec7a4a","rootDataFileId":-1,"md5":"8c572d40e8683f19cd32a44ce1c7f2b9","checksum":{"type":"MD5","value":"8c572d40e8683f19cd32a44ce1c7f2b9"},"tabularData":false,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}},{"description":"","label":"18ja003_fig2a_data.txt","restricted":false,"directoryLabel":"var/www/html/reports/18JA/18JA3","version":1,"datasetVersionId":143758,"dataFile":{"id":3231000,"persistentId":"doi:10.7910/DVN/X6XQTM/HW0C7J","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/HW0C7J","filename":"18ja003_fig2a_data.txt","contentType":"text/plain","friendlyType":"Plain Text","filesize":734,"description":"","storageIdentifier":"s3://dvn-cloud:166124bccae-e60c7234abe5","rootDataFileId":-1,"md5":"2aad2a6299d8294941e52ea38af51023","checksum":{"type":"MD5","value":"2aad2a6299d8294941e52ea38af51023"},"tabularData":false,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}},{"description":"","label":"18ja003_fig2a_image.pdf","restricted":false,"directoryLabel":"var/www/html/reports/18JA/18JA3","version":1,"datasetVersionId":143758,"dataFile":{"id":3230998,"persistentId":"doi:10.7910/DVN/X6XQTM/RMGBDA","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/RMGBDA","filename":"18ja003_fig2a_image.pdf","contentType":"application/pdf","friendlyType":"Adobe PDF","filesize":16063,"description":"","storageIdentifier":"s3://dvn-cloud:166124bccaa-796290346b56","rootDataFileId":-1,"md5":"ea8fe34ae3f45c4bf479b64335661ac5","checksum":{"type":"MD5","value":"ea8fe34ae3f45c4bf479b64335661ac5"},"tabularData":false,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}},{"description":"","label":"18ja003_fig2b_data.tab","restricted":false,"directoryLabel":"var/www/html/reports/18JA/18JA3","version":2,"datasetVersionId":143758,"dataFile":{"id":3230999,"persistentId":"doi:10.7910/DVN/X6XQTM/72OUU8","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/72OUU8","filename":"18ja003_fig2b_data.tab","contentType":"text/tab-separated-values","friendlyType":"Tab-Delimited","filesize":3452,"description":"","storageIdentifier":"s3://dvn-cloud:166124bccb8-90931aecfedd","originalFileFormat":"text/csv","originalFormatLabel":"Comma Separated Values","originalFileSize":3363,"originalFileName":"18ja003_fig2b_data.csv","UNF":"UNF:6:Lsq8qM0JPwAqpHXl4T4dLg==","rootDataFileId":-1,"md5":"5d294f3ac9e5f5c3915f61b6c6e69601","checksum":{"type":"MD5","value":"5d294f3ac9e5f5c3915f61b6c6e69601"},"tabularData":true,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}},{"description":"","label":"18ja003_fig2b_image.pdf","restricted":false,"directoryLabel":"var/www/html/reports/18JA/18JA3","version":1,"datasetVersionId":143758,"dataFile":{"id":3230997,"persistentId":"doi:10.7910/DVN/X6XQTM/E1DCST","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/E1DCST","filename":"18ja003_fig2b_image.pdf","contentType":"application/pdf","friendlyType":"Adobe PDF","filesize":14080,"description":"","storageIdentifier":"s3://dvn-cloud:166124bccb4-d58dfc79de52","rootDataFileId":-1,"md5":"f98599b6bbaf32ca21d60a54ca998000","checksum":{"type":"MD5","value":"f98599b6bbaf32ca21d60a54ca998000"},"tabularData":false,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}},{"description":"","label":"18ja003_fig4_data.tab","restricted":false,"directoryLabel":"var/www/html/reports/18JA/18JA3","version":2,"datasetVersionId":143758,"dataFile":{"id":3231001,"persistentId":"doi:10.7910/DVN/X6XQTM/7SOUHX","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/7SOUHX","filename":"18ja003_fig4_data.tab","contentType":"text/tab-separated-values","friendlyType":"Tab-Delimited","filesize":346,"description":"","storageIdentifier":"s3://dvn-cloud:166124bccc3-446de5c1dd2b","originalFileFormat":"text/csv","originalFormatLabel":"Comma Separated Values","originalFileSize":371,"originalFileName":"18ja003_fig4_data.csv","UNF":"UNF:6:1tJdBxTVtnhLRLzRaLefSA==","rootDataFileId":-1,"md5":"c6fd9a8c13389f0d9aeb5022199188be","checksum":{"type":"MD5","value":"c6fd9a8c13389f0d9aeb5022199188be"},"tabularData":true,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}},{"description":"","label":"18ja003_fig4_image.pdf","restricted":false,"directoryLabel":"var/www/html/reports/18JA/18JA3","version":1,"datasetVersionId":143758,"dataFile":{"id":3231002,"persistentId":"doi:10.7910/DVN/X6XQTM/JFYHRP","pidURL":"https://doi.org/10.7910/DVN/X6XQTM/JFYHRP","filename":"18ja003_fig4_image.pdf","contentType":"application/pdf","friendlyType":"Adobe PDF","filesize":13256,"description":"","storageIdentifier":"s3://dvn-cloud:166124bccbe-35ee204aee05","rootDataFileId":-1,"md5":"f7c92c610a351d6a23827dfa93e482fd","checksum":{"type":"MD5","value":"f7c92c610a351d6a23827dfa93e482fd"},"tabularData":false,"creationDate":"2018-09-25","publicationDate":"2018-09-25","fileAccessRequest":false}}],"citation":"I. H. Hutchinson, 2018, \"The mechanism of plasma electron hole transverse instability\", https://doi.org/10.7910/DVN/X6XQTM, Harvard Dataverse, V1, UNF:6:VCd4fG0yqyI1tXZGUsdMYA== [fileUNF]"}}