{"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":"95b7984b-bd8d-48f0-b5cf-c469d9fd17ff","name":"electron-swarm-parameters-c2h2-measurements-and-kinetic-calculations","title":"Electron swarm parameters in C2H2 - measurements and kinetic calculations","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 parameters (bulk drift velocity, bulk longitudinal component of the diffusion tensor, and effective ionization frequency) in C2H2 (acetylene) are investigated for a wide range of the reduced electric field by means of measurements and kinetic calculations. The dataset 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 flux drift velocity, bulk transversal component of the diffusion tensor, and effective steady-state Townsend ionization coefficient are given.\u003C\/p\u003E\n","url":"https:\/\/inptdat.de\/dataset\/electron-swarm-parameters-c2h2-measurements-and-kinetic-calculations","state":"Active","log_message":"Update to resource Electron swarm parameters in C2H2 - measured SST ionization coefficient","private":true,"revision_timestamp":"Tue, 02\/28\/2023 - 16:06","metadata_created":"Thu, 01\/30\/2020 - 09:39","metadata_modified":"Tue, 02\/28\/2023 - 16:06","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"4060ccfa-4a4e-4cdf-a275-92671699126e","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_measured-bulk-drift-velocity.csv","description":"\u003Cp\u003EMeasured bulk drift velocity W of electrons in acetylene (C2H2) 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_cor [10^{4} m\/s].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - measured bulk drift velocity","mimetype":"text\/csv","size":"549 bytes","created":"Thu, 01\/30\/2020 - 09:41","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"ee81c2b5-0de0-4fdb-931e-a6e172094f7e","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_measured-diffusion-coefficient.csv","description":"\u003Cp\u003EMeasured longitudinal component of the diffusion tensor times gas number density D_L N of electrons in acetylene (C2H2) at 293.15 K. The data table includes the reduced electric field, E\/N [Td], the measured data, (D_L N)_exptl [10^{24}m^{-1}s^{-1}], and the data corrected for systematic effects, (D_L N)_cor [10^{24}m^{-1}s^{-1}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - measured longitudinal diffusion coefficient","mimetype":"text\/csv","size":"545 bytes","created":"Thu, 01\/30\/2020 - 11:33","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"4522f899-ab45-4956-bb31-91c723c481e6","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_measured-ionization-frequency.csv","description":"\u003Cp\u003EMeasured reduced effective ionization frequency nu_eff\/N of electrons in acetylene (C2H2) at 293.15 K. The data table includes the reduced electric field, E\/N [Td], the measured data, (nu_eff\/N)_exptl [10^{-14}m^{3}\/s], and the data corrected for systematic effects, (nu_eff\/N)_cor [10^{-14}m^{3}\/s].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - measured ionization frequency","mimetype":"text\/csv","size":"473 bytes","created":"Thu, 01\/30\/2020 - 11:41","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"cf603b5c-3095-413a-874f-8bef6daae095","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_measured-SST-ionization-coefficient.csv","description":"\u003Cp\u003EReduced effective steady-state Townsend (SST) ionization coefficient alpha_eff\/N of electrons in acetylene (C2H2) 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^{-20}m^{2}], and the values calculated with the data corrected for systematic effects, (alpha_eff\/N)_cor [10^{-20}m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - measured SST ionization coefficient","mimetype":"text\/csv","size":"455 bytes","created":"Thu, 01\/30\/2020 - 11:47","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"38dd25f9-0fb7-4498-956d-1c2a92465f18","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_MC-results-for-C2H2.csv","description":"\u003Cp\u003ETabulated data of electron properties in acetylene (C2H2) at 293.15 K obtained by Monte Carlo simulations using the recommended electron collision cross section data of M.-Y. Song et al. , \u003Ca href=\u0022https:\/\/doi.org\/10.1063\/1.4976569\u0022\u003Ehttps:\/\/doi.org\/10.1063\/1.4976569\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the electron properties mean electron energy, U_e [eV],  flux drift velocity, w [m\/s], bulk drift velocity, W [m\/s], bulk longitudinal component of diffusion tensor times gas density, D_L N [m^{-1}s^{-1}],  bulk transverse component of diffusion tensor times gas density, D_T N [m^{-1}s^{-1}], reduced effective ionization frequency, nu_eff\/N [m^{3}\/s], and reduced effective steady-state Townsend ionization coefficient, alpha_eff\/N [m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - Monte Carlo simulation results","mimetype":"text\/csv","size":"3.46 KB","created":"Thu, 01\/30\/2020 - 11:56","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"7c082507-62cc-4bca-a900-17e1fcdc6238","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112-BEDG-results-for-C2H2.csv","description":"\u003Cp\u003ETabulated data of electron properties in acetylene (C2H2) at 293.15 K obtained by solving the electron Boltzmann equation (BE) in density gradient (DG) representation (method BE DG) using the recommended electron collision cross section data of M.-Y. Song et al., \u003Ca href=\u0022https:\/\/doi.org\/10.1063\/1.4976569\u0022\u003Ehttps:\/\/doi.org\/10.1063\/1.4976569\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the electron properties flux drift velocity, w [m\/s], bulk drift velocity, W [m\/s], gas number density times flux mobility, N mu_w [m^{-1}V^{-1}s^{-1}], gas number density times bulk mobility, N mu_W [m^{-1}V^{-1}s^{-1}], bulk longitudinal component of diffusion tensor times gas density, D_L N [m^{-1}s^{-1}],  bulk transverse component of diffusion tensor times gas density, D_T N [m^{-1}s^{-1}], flux longitudinal component of diffusion tensor times gas density, D_Lf N [m^{-1}s^{-1}],  flux transverse component of diffusion tensor times gas density, D_Tf N [m^{-1}s^{-1}], reduced effective ionization frequency, nu_eff\/N [m^{3}\/s], and reduced effective steady-state Townsend ionization coefficient, alpha_eff\/N [m^{2}].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - electron Boltzmann calculation results using BE DG method","mimetype":"text\/csv","size":"9.53 KB","created":"Thu, 01\/30\/2020 - 12:10","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"11ea46d8-7d49-4075-9fef-d402b358bd0d","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_BE0D-results-forC2H2.csv","description":"\u003Cp\u003ETabulated data of electron properties in acetylene (C2H2) at 293.15 K obtained by solving the electron Boltzmann equation (BE) in multiterm approximation for spatially homogeneous conditions (method BE 0D) using the recommended electron collision cross section data of M.-Y. Song et al., \u003Ca href=\u0022https:\/\/doi.org\/10.1063\/1.4976569\u0022\u003Ehttps:\/\/doi.org\/10.1063\/1.4976569\u003C\/a\u003E. The data table includes the reduced electric field, E\/N [Td], and the electron properties mean electron energy, U_e [eV],  flux drift velocity, w [m\/s], and reduced effective ionization frequency, nu_eff\/N [m^{3}\/s].\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 02\/28\/2023 - 16:06","name":"Electron swarm parameters in C2H2 - electron Boltzmann calculation results using BE 0D method","mimetype":"text\/csv","size":"11.77 KB","created":"Thu, 01\/30\/2020 - 14:38","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"},{"id":"ff09d590-0363-42cb-ab8f-aaed4aa05002","revision_id":"","url":"https:\/\/inptdat.de\/system\/files\/node112_BESST-results-for-C2H2.csv","description":"\u003Cp\u003ETabulated data of electron swarm parameters in acetylene (C2H2) 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 recommended electron collision cross section data of M.-Y. Song et al., \u003Ca href=\u0022https:\/\/doi.org\/10.1063\/1.4976569\u0022\u003Ehttps:\/\/doi.org\/10.1063\/1.4976569\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 - 16:06","name":"Electron swarm parameters in C2H2 - electron Boltzmann calculation results using BE SST method","mimetype":"text\/csv","size":"5.95 KB","created":"Thu, 01\/30\/2020 - 14:47","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 02\/28\/2023 - 16:06"}],"tags":[{"id":"02b8f23a-74ae-4f62-a99a-5d138f796aea","vocabulary_id":"2","name":"basic research"},{"id":"bd2592f7-24d0-4df9-94ec-6a6ee45dc5fc","vocabulary_id":"2","name":"electron swarm parameters"},{"id":"2cbcdcc9-424c-4cea-9cde-8c81b5c2f383","vocabulary_id":"2","name":"C2H2"}],"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. 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