{"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":"635c4fbc-f299-48c1-a843-c6dced54cf4c","name":"formation-mechanisms-striations-filamentary-dielectric-barrier-discharge-atmospheric","title":"Formation mechanisms of striations in a filamentary dielectric barrier discharge in atmospheric pressure argon - dataset","author":"DO NOT USE","author_email":"aleksandar.jovanovic@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 results of the modelling of a filamentary dielectric barrier discharge (DBD) in argon  at atmospheric pressure obtained using a time-dependent and spatially two-dimensional fluid-Poisson model in axisymmetric geometry are provided in this dataset.  The model was employed to investigate the formation mechanisms of the striations along the discharge channel in a one-sided DBD arrangement with a 1.5 mm gap powered by a sinusoidal high voltage applied at the metal electrode. The discharge conditions were chosen to resemble the experimental conditions for which striations have been observed. It was found that the striations form in both half-periods during the transient glow phase, which follows the streamer breakdown phase. The modelling results showed that the distinct striated structures feature local spatial maxima and minima in charged and excited particle densities, which were more pronounced during the positive polarity. Their formation was explained by a repetitive stepwise ionisation of metastable argon atoms and ionisation of excimers, causing a disturbance of the spatial distribution of charge carriers along the discharge channel. The results emphasise the importance of excited states and stepwise ionisation processes on the formation of repetitive ionisation waves, eventually leading to striations along the discharge channel.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/formation-mechanisms-striations-filamentary-dielectric-barrier-discharge-atmospheric","state":"Active","log_message":"Update to resource Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.13","private":true,"revision_timestamp":"Tue, 05\/09\/2023 - 21:47","metadata_created":"Tue, 04\/25\/2023 - 12:00","metadata_modified":"Tue, 05\/09\/2023 - 21:47","creator_user_id":"d52069c6-138a-4a56-9553-eddea8f72c53","type":"Dataset","resources":[{"id":"2cbae9f1-78bd-4501-9ad8-25458df48557","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure2.h5","description":"\u003Cp\u003EThe file contains the two datasets with temporal evolution of the electric current and voltages and spatiotemporal evolution of the electron number density and reduced electric field. Due to their size, the data are saved in binary hdf5 file. The file can be opened using any program that supports opening hdf5 files, such as HDF Viewer, Origin Pro, Matlab, or various libraries in Python. The current and voltage data are stored in a table where the first column is the time, the second, third and fourth columns are the applied, gap and memory voltages, respectively, and the last column is the electric current. The spatiotemporal evolution of the field is given in as a three-column form table in which for a given time in the first column all axial positions are varied in the second column, and the third and fourth columns contain the number density of electrons and the reduced electric field at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset1: \u0027Figure2_a\u0027\u003Cbr \/\u003E\nSize:  8546\u003Cbr \/\u003E\nStructured array:\u003Cbr \/\u003E\ncolumn 1: \u0027t [s]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: \u0027applied voltage [V]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: \u0027gap voltage [V]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 4: \u0027memory voltage [V]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 5: \u0027current [A]\u0027: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n\u003Cp\u003EDataset2: \u0027Figure2_b-c\u0027:\u003Cbr \/\u003E\nSize:  264528\u003Cbr \/\u003E\nStructured array:\u003Cbr \/\u003E\ncolumn 1: \u0027t [s]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: \u0027z [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: \u0027[e] [m^-3]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 4: \u0027reduced electric field [Td]\u0027: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n\u003Cp\u003ENote that the same data zoomed into different time ranges was presented in Figures 3 and 12.\u003C\/p\u003E\n","format":"data","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.2","mimetype":"application\/octet-stream","size":"8.4 MB","created":"Tue, 04\/25\/2023 - 10:29","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"e23bf086-bc55-4350-8926-a3b920f1cae3","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure4.h5","description":"\u003Cp\u003EThe spatial profiles of the electron number density for three characteristic times during the streamer phase. Due to their size, the data are saved in binary hdf5 file. The file can be opened using any program that supports opening hdf5 files, such as HDF Viewer, Origin Pro, Matlab, or various libraries in python. The data are stored as a three-column form table in which the radial position in the first column is varied for each axial position in the second column and the following columns contain the number density of electrons for corresponding positions at the given times. Note that NaN data occur for the spatial points outside the computational domain.\u003C\/p\u003E\n\u003Cp\u003EDataset: \u0027Figure4_a-c\u0027\u003Cbr \/\u003E\nSize: 777051\u003Cbr \/\u003E\nStructured array:\u003Cbr \/\u003E\ncolumn 1: \u0027r [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: \u0027z [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: \u0027[e] [m^-3] at 50.40 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 4: \u0027[e] [m^-3] at 50.48 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 5: \u0027[e] [m^-3] at 50.50 microseconds\u0027: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"data","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.4","mimetype":"application\/octet-stream","size":"29.65 MB","created":"Tue, 04\/25\/2023 - 10:51","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"8de3a333-fffc-49c8-ad2b-eca3ef530fd6","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure5_0.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and mean electron energy along the symmetry axis at three characteristic times during the streamer phase. The table contains the axial position in the first column, and number densities of the particles and the mean electron energy for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027[Ar^*] [m^-3]  at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027[Ar^+] [m^-3] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027[Ar_2^*] [m^-3] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027[Ar_2^+] [m^-3] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027[e] [m^-3] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027u_e [eV] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027[Ar^*] [m^-3]  at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027[Ar^+] [m^-3] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027[Ar_2^*] [m^-3] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027[Ar_2^+] [m^-3] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027[e] [m^-3] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027u_e [eV] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 14: \u0027[Ar^*] [m^-3]  at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 15: \u0027[Ar^+] [m^-3] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 16: \u0027[Ar_2^*] [m^-3] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 17: \u0027[Ar_2^+] [m^-3] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 18: \u0027[e] [m^-3] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 19: \u0027u_e [eV] at 50.50 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.5","mimetype":"text\/csv","size":"131 KB","created":"Tue, 04\/25\/2023 - 11:24","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"679b53fc-850c-44f8-a332-8f846e187f20","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure6_0.csv","description":"\u003Cp\u003ESpatial profiles of the rates of electron production, and reduced electric field along the symmetry axis at three characteristic times during the streamer phase. The table contains the axial position in the first column, and rates and the reduced electric field for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027direct ionsiation [m^-3 s^-1] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027stepwise ionisation [m^-3 s^-1]  at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027excimer ionsiation [m^-3 s^-1] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027chemo-ionisation [m^-3 s^-1] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027dissociative recombination [m^-3 s^-1] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027reduced electric field [Td] at 50.40 microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027direct ionsiation [m^-3 s^-1] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027stepwise ionisation [m^-3 s^-1] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027excimer ionsiation [m^-3 s^-1] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027chemo-ionisation [m^-3 s^-1] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027dissociative recombination [m^-3 s^-1] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027reduced electric field [Td] at 50.48 microseconds\u0027\u003Cbr \/\u003E\ncolumn 14: \u0027direct ionsiation [m^-3 s^-1] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 15: \u0027stepwise ionisation [m^-3 s^-1]  at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 16: \u0027excimer ionsiation [m^-3 s^-1] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 17: \u0027chemo-ionisation [m^-3 s^-1] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 18: \u0027dissociative recombination [m^-3 s^-1] at 50.50 microseconds\u0027\u003Cbr \/\u003E\ncolumn 19: \u0027reduced electric field [Td] at 50.50 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.6","mimetype":"text\/csv","size":"234.83 KB","created":"Tue, 04\/25\/2023 - 11:40","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"9b6f0575-694f-4397-947c-0ffbd97a2fe9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure7.h5","description":"\u003Cp\u003EThe spatial profiles of the electron number density for four characteristic times during the transient glow phase. Due to their size, the data are saved in binary hdf5 file. The file can be opened using any program that supports opening hdf5 files, such as HDF Viewer, Origin Pro, Matlab, or various libraries in python. The data are stored as a three-column form table in which the radial position in the first column is varied for each axial position in the second column and the following columns contain the number density of electrons for corresponding positions at the given times. Note that NaN data occur for the spatial points outside the computational domain.\u003C\/p\u003E\n\u003Cp\u003EDataset: \u0027Figure7_a-d\u0027\u003Cbr \/\u003E\nSize: 777051\u003Cbr \/\u003E\nStructured array:\u003Cbr \/\u003E\ncolumn 1: \u0027r [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: \u0027z [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: \u0027[e] [m^-3] at 51.1 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 4: \u0027[e] [m^-3] at 51.6 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 5: \u0027[e] [m^-3] at 51.8 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 6: \u0027[e] [m^-3] at 52.0 microseconds\u0027: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"data","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.7","mimetype":"application\/octet-stream","size":"35.57 MB","created":"Tue, 04\/25\/2023 - 11:49","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"148a3a3b-335b-42f3-b305-070b9581a79f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure8_0.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species along the symmetry axis at four characteristic times during the transient glow phase. The table contains the axial position in the first column, and number densities of the particles for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027[Ar^*] [m^-3] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027[Ar^+] [m^-3] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027[Ar_2^*] [m^-3] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027[Ar_2^+] [m^-3] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027[e] [m^-3] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027[Ar^*] [m^-3] at 51.6microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027[Ar^+] [m^-3] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027[Ar_2^*] [m^-3] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027[Ar_2^+] [m^-3] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027[e] [m^-3] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027[Ar^*] [m^-3] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027[Ar^+] [m^-3] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 14: \u0027[Ar_2^*] [m^-3] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 15: \u0027[Ar_2^+] [m^-3] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 16: \u0027[e] [m^-3] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 17: \u0027[Ar^*] [m^-3] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 18: \u0027[Ar^+] [m^-3] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 19: \u0027[Ar_2^*] [m^-3] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 20: \u0027[Ar_2^+] [m^-3] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 21: \u0027[e] [m^-3] at 52.0 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.8","mimetype":"text\/csv","size":"257.57 KB","created":"Tue, 04\/25\/2023 - 12:07","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"8a05d532-b921-41c0-a284-2012ad653266","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure9_0.csv","description":"\u003Cp\u003ESpatial profiles of the reduced electric field, mean electron energy and space charge density along the symmetry axis at four characteristic times during the transient glow phase. The table contains the axial position in the first column, and the reduced electric field, mean electron energy and space charge density for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027reduced electric field [Td] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027mean electron energy [eV]  at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027space charge density [C m^-3] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027reduced electric field [Td] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027mean electron energy [eV]  at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027space charge density [C m^-3] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027reduced electric field [Td] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027mean electron energy [eV]  at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027space charge density [C m^-3] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027reduced electric field [Td] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027mean electron energy [eV]  at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027space charge density [C m^-3] at 52.0 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.9","mimetype":"text\/csv","size":"159.71 KB","created":"Tue, 04\/25\/2023 - 12:14","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"91a19835-1adc-4fa7-9518-32f16bee1bdd","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure10_0.csv","description":"\u003Cp\u003ESpatial profiles of the rates of electron production, and divergence of the electric flux along the symmetry axis at four characteristic times during the transient glow phase. The table contains the axial position in the first column, and rates and the divergence of the flux for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027direct ionsiation [m^-3 s^-1] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027stepwise ionisation [m^-3 s^-1]  at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027excimer ionsiation [m^-3 s^-1] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027chemo-ionisation [m^-3 s^-1] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027dissociative recombination [m^-3 s^-1] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027divergence of electron flux [m^-3 s^-1] at 51.1 microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027direct ionsiation [m^-3 s^-1] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027stepwise ionisation [m^-3 s^-1]  at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027excimer ionsiation [m^-3 s^-1] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027chemo-ionisation [m^-3 s^-1] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027dissociative recombination [m^-3 s^-1] at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027divergence of electron flux [m^-3 s^-1]  at 51.6 microseconds\u0027\u003Cbr \/\u003E\ncolumn 14: \u0027direct ionsiation [m^-3 s^-1] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 15: \u0027stepwise ionisation [m^-3 s^-1]  at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 16: \u0027excimer ionsiation [m^-3 s^-1] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 17: \u0027chemo-ionisation [m^-3 s^-1] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 18: \u0027dissociative recombination [m^-3 s^-1] at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 19: \u0027divergence of electron flux [m^-3 s^-1]  at 51.8 microseconds\u0027\u003Cbr \/\u003E\ncolumn 20: \u0027direct ionsiation [m^-3 s^-1] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 21: \u0027stepwise ionisation [m^-3 s^-1]  at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 22: \u0027excimer ionsiation [m^-3 s^-1] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 23: \u0027chemo-ionisation [m^-3 s^-1] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 24: \u0027dissociative recombination [m^-3 s^-1] at 52.0 microseconds\u0027\u003Cbr \/\u003E\ncolumn 25: \u0027divergence of electron flux [m^-3 s^-1]  at 52.0 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.10","mimetype":"text\/csv","size":"309.2 KB","created":"Tue, 04\/25\/2023 - 12:27","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"3d71e1c3-2f30-4438-aa3b-8144cbeb9ad6","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure11.h5","description":"\u003Cp\u003EAbel-transformed distribution of the electron density at the time of the most intense striations. Due to file size, the data are saved in binary hdf5 file. The file can be opened using any program that supports opening hdf5 files, such as HDF Viewer, Origin Pro, Matlab, or various libraries in python. The data are stored as a three-column form table in which the radial position in the first column is varied for each axial position in the second column and the following column contains the Abel-transformed electron density for corresponding positions. Note that NaN data occur for the spatial points outside the computational domain.\u003C\/p\u003E\n\u003Cp\u003EDataset: \u0027Figure11\u0027\u003Cbr \/\u003E\nSize: 60802\u003Cbr \/\u003E\nStructured array:\u003Cbr \/\u003E\ncolumn 1: \u0027r [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: \u0027z [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: \u0027Abel transformed [e] [m^-3] at 52.0 microseconds\u0027: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"data","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.11","mimetype":"application\/octet-stream","size":"1.39 MB","created":"Tue, 04\/25\/2023 - 12:35","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"6e9cd8d2-64f1-4f4f-976c-6d2ce2de8a4b","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure13.h5","description":"\u003Cp\u003EThe spatial profiles of the electron number density for three characteristic times during the discharge in the negative half-period. The data are saved in binary hdf5 file due to their size. The file can be opened using any program that supports opening hdf5 files, such as HDF Viewer, Origin Pro, Matlab, or various libraries in python. The data are stored as a three-column form table in which the radial position in the first column is varied for each axial position in the second column and the following columns contain the number density of electrons for corresponding positions at the given times. Note that NaN data occur for the spatial points outside the computational domain.\u003C\/p\u003E\n\u003Cp\u003EDataset: \u0027Figure13_a-c\u0027\u003Cbr \/\u003E\nSize: 777051\u003Cbr \/\u003E\nStructured array:\u003Cbr \/\u003E\ncolumn 1: \u0027r [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: \u0027z [m]\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: \u0027[e] [m^-3] at 56.700 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 4: \u0027[e] [m^-3] at 56.781 microseconds\u0027: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 5: \u0027[e] [m^-3] at 57.000 microseconds\u0027: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"data","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.13","mimetype":"application\/octet-stream","size":"29.65 MB","created":"Tue, 04\/25\/2023 - 13:32","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"256f1937-fe43-46dd-b637-9e0a4fc2671e","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure14.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and mean electron energy along the symmetry axis at three characteristic times during the discharge in the negative half-period. The table contains the axial position in the first column, and number densities of the particles and the mean electron energy for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027[Ar^*] [m^-3] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027[Ar^+] [m^-3] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027[Ar_2^*] [m^-3] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027[Ar_2^+] [m^-3] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027[e] [m^-3] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027u_e [eV] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027[Ar^*] [m^-3] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027[Ar^+] [m^-3] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027[Ar_2^*] [m^-3] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027[Ar_2^+] [m^-3] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027[e] [m^-3] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027u_e [eV] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 14: \u0027[Ar^*] [m^-3] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 15: \u0027[Ar^+] [m^-3] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 16: \u0027[Ar_2^*] [m^-3] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 17: \u0027[Ar_2^+] [m^-3] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 18: \u0027[e] [m^-3] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 19: \u0027u_e [eV] at 57.000 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.14","mimetype":"text\/csv","size":"233.06 KB","created":"Tue, 04\/25\/2023 - 13:52","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"},{"id":"48fa33fb-2cc9-4ae5-b5a4-75b665a68fd3","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node669_figure15_0.csv","description":"\u003Cp\u003ESpatial profiles of the rates of electron production, and reduced electric field along the symmetry axis at three characteristic times during the discharge in the negative half-period. The table contains the axial position in the first column, and rates and the reduced electric field for each time in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: \u0027z [m]\u0027\u003Cbr \/\u003E\ncolumn 2: \u0027direct ionsiation [m^-3 s^-1] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 3: \u0027stepwise ionisation [m^-3 s^-1] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 4: \u0027excimer ionsiation [m^-3 s^-1] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 5: \u0027chemo-ionisation [m^-3 s^-1] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 6: \u0027dissociative recombination [m^-3 s^-1] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 7: \u0027reduced electric field [Td] at 56.700 microseconds\u0027\u003Cbr \/\u003E\ncolumn 8: \u0027direct ionsiation [m^-3 s^-1] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 9: \u0027stepwise ionisation [m^-3 s^-1] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 10: \u0027excimer ionsiation [m^-3 s^-1] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 11: \u0027chemo-ionisation [m^-3 s^-1] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 12: \u0027dissociative recombination [m^-3 s^-1] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 13: \u0027reduced electric field [Td] at 56.781 microseconds\u0027\u003Cbr \/\u003E\ncolumn 14: \u0027direct ionsiation [m^-3 s^-1] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 15: \u0027stepwise ionisation [m^-3 s^-1] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 16: \u0027excimer ionsiation [m^-3 s^-1] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 17: \u0027chemo-ionisation [m^-3 s^-1] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 18: \u0027dissociative recombination [m^-3 s^-1] at 57.000 microseconds\u0027\u003Cbr \/\u003E\ncolumn 19: \u0027reduced electric field [Td] at 57.000 microseconds\u0027\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 04\/25\/2023 - 15:20","name":"Formation mechanisms of striations in a filamentary DBD in atmospheric pressure Ar-Fig.15","mimetype":"text\/csv","size":"234.85 KB","created":"Tue, 04\/25\/2023 - 14:05","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 04\/25\/2023 - 15:20"}],"tags":[{"id":"8dde877f-9b50-4dd2-a90d-8f69ad86a950","vocabulary_id":"2","name":"DBD"},{"id":"0487700f-e4dd-445d-a0bb-b46d40cc2563","vocabulary_id":"2","name":"striations"},{"id":"95452d90-ed0c-41cc-a020-93759a51d243","vocabulary_id":"2","name":"fluid modelling"},{"id":"4422fa94-b35f-4970-9732-81fb95852746","vocabulary_id":"2","name":"streamer discharge"}],"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\u003EMasaryk University\u003Cbr \/\u003E\n\u003Cstrong\u003EPlasma diagnostics and modelling group\u003C\/strong\u003E\u003Cbr \/\u003E\nKotl\u00e1\u0159sk\u00e1 267\/2\u003Cbr \/\u003E\n611 37 Brno\u003Cbr \/\u003E\nCZECH REPUBLIC\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022http:\/\/www.physics.muni.cz\/en\/research\/research-groups\/pdm\u0022\u003EHomepage\u003C\/a\u003E\u003Cbr \/\u003E\n\u003Cspan class=\u0022spamspan\u0022\u003E\u003Cspan class=\u0022u\u0022\u003Ehoder\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\u003Ephysics\u003Cspan class=\u0022t\u0022\u003E [punkt] \u003C\/span\u003Emuni\u003Cspan class=\u0022t\u0022\u003E [punkt] \u003C\/span\u003Ecz\u003C\/span\u003E\u003C\/span\u003E\u003C\/p\u003E\n","id":"be107fac-c175-4b50-83a1-4d8cb7d894ef","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/muni-sci.png","title":"MUNI SCI PDM","name":"group\/muni-sci-pdm"}]}]}