{"help":"Return the metadata of a dataset (package) and its resources. :param id: the id or name of the dataset :type id: string","success":true,"result":[{"id":"059a3b9f-a83d-4b84-8fb6-bc21d01df28e","name":"electron-swarm-transport-coefficients-co-measurements-and-kinetic-studies","title":"Electron swarm transport coefficients in CO - measurements and kinetic studies","author_email":"loffhagen@inp-greifswald.de","maintainer":"INPTDAT \u2013 The Data Platform for Plasma Technology","maintainer_email":"wissenschafts-it@inp-greifswald.de","license_title":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/","notes":"\u003Cp\u003EThe electron swarm transport coefficients (bulk drift velocity, bulk longitudinal component of the diffusion tensor, and effective ionization frequency) in CO are investigated for a wide range of the reduced electric field by means of measurements and kinetic calculations. The set of data contains results of measurements in a scanning drift tube apparatus under time-of-flight conditions as well as of kinetic swarm calculations using solutions of the electron Boltzmann equation and Monte Carlo simulations. In addition to the bulk drift velocity, bulk longitudinal component of the diffusion tensor, and effective ionization frequency, results of the average electron energy, flux drift velocity, flux longitudinal component of the diffusion tensor, flux and bulk transversal component of the diffusion tensor, bulk longitudinal and transversal characteristic energy as well as the effective steady-state Townsend ionization coefficient are given.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/electron-swarm-transport-coefficients-co-measurements-and-kinetic-studies","state":"Active","log_message":"Update to resource Electron swarm transport coefficients in CO - Monte Carlo simulation results under hydrodynamic conditions ","private":true,"revision_timestamp":"Tue, 02\/28\/2023 - 16:05","metadata_created":"Sun, 02\/12\/2023 - 21:40","metadata_modified":"Tue, 02\/28\/2023 - 16:05","creator_user_id":"a1ed6607-e1e5-44e8-b6ca-3c572f17ae61","type":"Dataset","resources":[{"id":"3ad89e2e-c24a-4064-9256-bcd83fc846fc","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548-measured-bulk-drift-velocity.csv","description":"\u003Cp\u003EMeasured bulk drift velocity W of electrons in carbon monoxide (CO) at 293.15 K. The data table includes the reduced electric field, E\/N [Td], the measured data, W_exptl [10^{4} m\/s], and the data corrected for systematic effects, W_corr [10^{4} m\/s].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - measured bulk drift velocity","mimetype":"text\/csv","size":"599 bytes","created":"Tue, 05\/10\/2022 - 15:39","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"8e0884bc-458b-4877-a3cc-cac927653205","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_measured-diffusion-coefficient.csv","description":"\u003Cp\u003EMeasured longitudinal component of the diffusion tensor times gas number density D_L N of electrons in carbon monoxide (CO) at 293.15 K. The data table includes the reduced electric field, E\/N [Td], the measured data, (D_L N)_exptl [10^{23}m^{-1}s^{-1}], and the data corrected for systematic effects, (D_L N)_corr [10^{23}m^{-1}s^{-1}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - measured bulk longitudinal diffusion coefficient","mimetype":"text\/csv","size":"557 bytes","created":"Tue, 05\/10\/2022 - 16:03","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"42460126-7b70-4353-a5d9-75e0127d7357","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_measured-ionization-frequency.csv","description":"\u003Cp\u003EMeasured reduced effective ionization frequency nu_eff\/N of electrons in carbon monoxide (CO) at 293.15 K. The data table includes the reduced electric field, E\/N [Td], the measured data, (nu_eff\/N)_exptl [10^{-16} m^{3}\/s], and the data corrected for systematic effects, (nu_eff\/N)_corr [10^{-16} m^{3}\/s].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - measured ionization frequency","mimetype":"text\/csv","size":"346 bytes","created":"Tue, 05\/10\/2022 - 16:10","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"040ae14b-4fd0-4fd7-a657-7af1851b1c3f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_measured-SST-ionization-coefficient.csv","description":"\u003Cp\u003EReduced effective steady-state Townsend ionization coefficient alpha_eff\/N of electrons in carbon monoxide (CO) at 293.15 K calculated using the measured values of W, D_L and nu_eff. The data table includes the reduced electric field, E\/N [Td], the values calculated with the measured data, (alpha_eff\/N)_exptl [10^{-22} m^{2}], and the values calculated with the data corrected for systematic effects, (alpha_eff\/N)_corr [10^{-22} m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - measured SST ionization coefficient ","mimetype":"text\/csv","size":"355 bytes","created":"Tue, 05\/10\/2022 - 16:17","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"a2541ab4-defb-46e6-b68f-c735da1ef5a5","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_MCTOFresults-for-CO20220503.csv","description":"\u003Cp\u003ETabulated data of electron swarm transport coefficients in carbon monoxide (CO) at 293.15 K obtained by Monte Carlo simulations under hydrodynamic conditions using the electron collision cross section data released by S. Biagi in Magboltz v11.11 (edition of 25 Jan 2021), \u003Ca href=\u0022https:\/\/magboltz.web.cern.ch\/magboltz\/\u0022\u003Ehttps:\/\/magboltz.web.cern.ch\/magboltz\/\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the electron swarm transport coefficients mean energy, U_e [eV], bulk longitudinal characteristic energy, D_L\/mu [eV], bulk transversal characteristic energy, D_T\/mu [eV], flux drift velocity, W^* [m\/s], bulk drift velocity, W [m\/s], gas density times flux longitudinal diffusion coefficient, N D_L^* [m^{-1} s^{-1}], gas density times bulk longitudinal diffusion coefficient, N D_L [m^{-1} s^{-1}], gas density times flux transverse diffusion coefficient, N D_T^* [m^{-1} s^{-1}], gas density times bulk transverse diffusion coefficient, N D_T [m^{-1} s^{-1}], ionization rate coefficient, k_i [m^{3}\/s], attachment rate coefficient, k_a [m^{3}\/s], and reduced effective SST ionization coefficient, alpha_eff\/N(Hydro) [m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - Monte Carlo simulation results under hydrodynamic conditions ","mimetype":"text\/csv","size":"4.88 KB","created":"Tue, 05\/10\/2022 - 16:23","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"9417e530-ce3d-45da-a2ea-3d23e184512f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_MCSSTresults-for-CO20220503.csv","description":"\u003Cp\u003ETabulated data of electron swarm transport coefficients in carbon monoxide (CO) at 293.15 K obtained by Monte Carlo simulations for steady-state Townsend (SST) conditions using the electron collision cross section data released by S. Biagi in Magboltz v11.11 (edition of 25 Jan 2021), \u003Ca href=\u0022https:\/\/magboltz.web.cern.ch\/magboltz\/\u0022\u003Ehttps:\/\/magboltz.web.cern.ch\/magboltz\/\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the reduced effective SST ionization coefficient, alpha_eff\/N(SST) [m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - Monte Carlo simulation results for steady-state Townsend conditions ","mimetype":"text\/csv","size":"530 bytes","created":"Tue, 05\/10\/2022 - 16:26","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"6263e2a0-f0ae-46e6-a09b-c5a3df52b54d","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_BEDGresults-for-CO20220503.csv","description":"\u003Cp\u003ETabulated data of electron swarm transport coefficients in carbon monoxide (CO) at 293.15 K obtained by solving the electron Boltzmann equation (BE) in density gradient (DG) representation (method BE DG) using the electron collision cross section data released by S. Biagi in Magboltz v11.11 (edition of 25 Jan 2021), \u003Ca href=\u0022https:\/\/magboltz.web.cern.ch\/magboltz\/\u0022\u003Ehttps:\/\/magboltz.web.cern.ch\/magboltz\/\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the electron swarm transport coefficients mean energy, U_e [eV], bulk longitudinal characteristic energy, D_L\/mu [eV], bulk transversal characteristic energy, D_T\/mu [eV], flux drift velocity, W^* [m\/s], bulk drift velocity, W [m\/s], gas density times flux longitudinal diffusion coefficient, N D_L^* [m^{-1} s^{-1}], gas density times bulk longitudinal diffusion coefficient, N D_L [m^{-1} s^{-1}], gas density times flux transverse diffusion coefficient, N D_T^* [m^{-1} s^{-1}], gas density times bulk transverse diffusion coefficient, N D_T [m^{-1} s^{-1}], ionization rate coefficient, k_i [m^{3}\/s], attachment rate coefficient, k_a [m^{3}\/s], and reduced effective SST ionization coefficient, alpha_eff\/N(Hydro) [m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - electron Boltzmann calculation results using BE DG method ","mimetype":"text\/csv","size":"18.52 KB","created":"Tue, 05\/10\/2022 - 16:33","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"e0e0aa9c-0926-47ce-91a8-ac0c3293056e","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_BEMT-results-for-CO.csv","description":"\u003Cp\u003ETabulated data of electron swarm transport coefficients in carbon monoxide (CO) at 293.15 K obtained by solving the electron Boltzmann equation (BE) in multiterm approximation for spatially homogeneous conditions (method BE MT) using the electron collision cross section data released by S. Biagi in Magboltz v11.11 (edition of 25 Jan 2021), \u003Ca href=\u0022https:\/\/magboltz.web.cern.ch\/magboltz\/\u0022\u003Ehttps:\/\/magboltz.web.cern.ch\/magboltz\/\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the electron swarm transport coefficients mean energy, U_e [eV], gas density times flux transverse diffusion coefficient, N D_T^* [m^{-1} s^{-1}], flux drift velocity, W^* [m\/s], ionization rate coefficient, k_i [m^{3}\/s], and attachment rate coefficient, k_a [m^{3}\/s].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - electron Boltzmann calculation results using BE MT method","mimetype":"text\/csv","size":"16.05 KB","created":"Tue, 05\/10\/2022 - 16:37","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"},{"id":"6f2bed55-d278-4c06-9bae-e143c755d3b3","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node548_BESST-results-for-CO.csv","description":"\u003Cp\u003ETabulated data of electron swarm transport coefficients in carbon monoxide (CO) at 293.15 K obtained by solving the electron Boltzmann equation (BE) in multiterm approximation for steady-state Townsend (SST) conditions (method BE SST) using the electron collision cross section data released by S. Biagi in Magboltz v11.11 (edition of 25 Jan 2021), \u003Ca href=\u0022https:\/\/magboltz.web.cern.ch\/magboltz\/\u0022\u003Ehttps:\/\/magboltz.web.cern.ch\/magboltz\/\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the reduced effective SST ionization coefficient, alpha_eff\/N [m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:05","name":"Electron swarm transport coefficients in CO - electron Boltzmann calculation results using BE SST method","mimetype":"text\/csv","size":"3.89 KB","created":"Tue, 05\/10\/2022 - 16:42","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:05"}],"tags":[{"id":"02b8f23a-74ae-4f62-a99a-5d138f796aea","vocabulary_id":"2","name":"basic research"},{"id":"9957e2bb-1fd5-44ca-9c59-b653a468f4a7","vocabulary_id":"2","name":"electron swarm transport coefficients"},{"id":"db86a63c-ea20-44a6-9429-705d338a1228","vocabulary_id":"2","name":"CO"}],"groups":[{"description":"\u003Cp\u003E\u003Cstrong\u003ELeibniz Institute for Plasma Science and Technology\u003C\/strong\u003E\u003Cbr \/\u003E\nFelix-Hausdorff-Str. 2\u003Cbr \/\u003E\n17489 Greifswald\u003Cbr \/\u003E\nGERMANY\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/www.inp-greifswald.de\/en\/\u0022\u003Ehttps:\/\/www.inp-greifswald.de\/en\/\u003C\/a\u003E\u003Cbr \/\u003E\n\u003Cspan class=\u0022spamspan\u0022\u003E\u003Cspan class=\u0022u\u0022\u003Ewelcome\u003C\/span\u003E\u003Cimg class=\u0022spam-span-image\u0022 alt=\u0022at\u0022 width=\u002210\u0022 src=\u0022\/sites\/all\/modules\/spamspan\/image.gif\u0022 \/\u003E\u003Cspan class=\u0022d\u0022\u003Einp-greifswald\u003Cspan class=\u0022t\u0022\u003E [punkt] \u003C\/span\u003Ede\u003C\/span\u003E\u003C\/span\u003E\u003C\/p\u003E\n\u003Cp align=\u0022justify\u0022\u003EThe Leibniz Institute for Plasma Science and Technology (INP) is the largest non-university institute in the field of low temperature plasmas, their basics and technical applications in Europe. The institute carries out research and development from idea to prototype. The topics focus on the needs of the market. At present, plasmas for materials and energy as well as for environment and health are the focus of interest. \u003C\/p\u003E\n","id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/inp.png","title":"INP","name":"group\/inp"},{"description":"\u003Cp\u003E\u003Cstrong\u003EWigner Research Centre for Physics\u003C\/strong\u003E\u003Cbr \/\u003E\nKonkoly-Thege Mikl\u00f3s \u00fat 29-33\u003Cbr \/\u003E\n1121 Budapest\u003Cbr \/\u003E\nHUNGARY\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/wigner.hu\/en\u0022\u003Ehttps:\/\/wigner.hu\/en\u003C\/a\u003E\u003Cbr \/\u003E\n\u003Cspan class=\u0022spamspan\u0022\u003E\u003Cspan class=\u0022u\u0022\u003Ewigner\u003C\/span\u003E\u003Cimg class=\u0022spam-span-image\u0022 alt=\u0022at\u0022 width=\u002210\u0022 src=\u0022\/sites\/all\/modules\/spamspan\/image.gif\u0022 \/\u003E\u003Cspan class=\u0022d\u0022\u003Ewigner\u003Cspan class=\u0022t\u0022\u003E [punkt] \u003C\/span\u003Ehu\u003C\/span\u003E\u003C\/span\u003E\u003C\/p\u003E\n","id":"3f614647-cbdc-47d1-8488-61d08baf0974","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/wigner.png","title":"Wigner","name":"group\/wigner"},{"description":"\u003Cp\u003ERuhr Uni\u00adver\u00adsi\u00adty Bo\u00adchum\u003Cbr \/\u003E\n\u003Cstrong\u003EChair of Applied Electrodynamics and Plasma Technology AEPT\u003C\/strong\u003E\u003Cbr \/\u003E\n44780 Bo\u00adchum\u003Cbr \/\u003E\nGERMANY\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/www.aept.ruhr-uni-bochum.de\/en\/\u0022\u003Ehttps:\/\/www.aept.ruhr-uni-bochum.de\/en\/\u003C\/a\u003E\u003C\/p\u003E\n","id":"53ad023d-3956-44db-b33e-9d1e3d5ae04d","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/aept.png","title":"AEPT","name":"group\/aept"},{"description":"\u003Cp\u003E\u003Cstrong\u003EInstitute of Physics Belgrade\u003C\/strong\u003E\u003Cbr \/\u003E\nUniversity of Belgrade\u003Cbr \/\u003E\nPregrevica 118\u003Cbr \/\u003E\nBelgrade\u003Cbr \/\u003E\nSERBIA\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/www.ipb.ac.rs\/en\/home-en\/\u0022\u003Ehttps:\/\/www.ipb.ac.rs\/en\/home-en\/\u003C\/a\u003E\u003C\/p\u003E\n","id":"727e6668-acb5-4e0e-9bb4-ed74dfb28092","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/ipb.png","title":"IPB","name":"group\/ipb"},{"description":"\u003Cp\u003EInstituto de Plasmas e Fus\u00e3o Nuclear\u003Cbr \/\u003E\n\u003Cstrong\u003EInstituto Superior T\u00e9cnico\u003C\/strong\u003E\u003Cbr \/\u003E\nUniversidade de Lisboa\u003Cbr \/\u003E\nAv. Rovisco Pais\u003Cbr \/\u003E\nLisbon, 1049-001\u003Cbr \/\u003E\nPORTUGAL\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/tecnico.ulisboa.pt\/en\/\u0022\u003Ehttps:\/\/tecnico.ulisboa.pt\/en\/\u003C\/a\u003E\u003C\/p\u003E\n","id":"534f9f48-596d-4286-898a-3eb3f7dce0a3","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/ist.png","title":"IST","name":"group\/ist"}]}]}