{"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":"b5754c4f-21dd-44c9-aa35-9352c049afd2","name":"discharge-modes-self-pulsing-discharges-argon-atmospheric-pressure-dataset","title":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - 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 modelling study of self-pulsing discharges in pure argon at atmospheric pressure in a 1.5 mm gas gap are provided in this dataset. The study investigates the interaction between the electrical circuit and the actual plasma characteristics. A time-dependent, spatially one-dimensional fluid-Poisson model coupled with an equivalent circuit equation is applied to analyse the impact of circuit parameters like resistance and applied negative DC high voltage on basic discharge properties. This includes the analysis of the spatio-temporal development of the densities of charge carriers and excited species, the electric field and ionisation rates in combination with the synchronised electrical quantities like discharge current, discharge voltage and self-pulsing frequency. The study identifies three distinct self-pulsing modes of the discharge, i.e., a transient spark, a transient glow and a modulated DC glow mode. The transition between these modes is related to different recharging times of the circuit capacitance for different external resistances in series with the gas gap, which leads to changes in the predominance of the different ionisation processes together with the crucial impact of pre-ionisation on the discharge inception. These insights provide essential knowledge on tunability within a selection of self-pulsing DC discharge modes for generating non-thermal plasma with desired effects, e.g. for material processing and environmental or medical applications.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/discharge-modes-self-pulsing-discharges-argon-atmospheric-pressure-dataset","state":"Active","log_message":"Update to resource Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.12","private":true,"revision_timestamp":"Tue, 07\/15\/2025 - 15:56","metadata_created":"Wed, 04\/30\/2025 - 16:33","metadata_modified":"Tue, 07\/15\/2025 - 15:56","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"07126c44-1bfc-42ee-9407-a679a08518c8","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure3a.csv","description":"\u003Cp\u003EThe temporal variation of the discharge voltage (U), electric current (I) and voltage drop at the resistor (IR) in TSM. The data are given in a form of table where the first column represents time, the second column is the voltage, the third column is the electric current and the fourth is the voltage drop at the resistor (IR).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.3(a)","mimetype":"text\/csv","size":"652.33 KB","created":"Wed, 05\/28\/2025 - 11:02","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"49fe11c3-233b-4edc-a36e-0147865c7c2b","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure3b.csv","description":"\u003Cp\u003EThe temporal variation of the discharge voltage (U), electric current (I) and voltage drop at the resistor (IR) in TGM. The data are given in a form of table where the first column represents time, the second column is the voltage, the third column is the electric current and the fourth is the voltage drop at the resistor (IR).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.3(b)","mimetype":"text\/csv","size":"194.57 KB","created":"Wed, 05\/28\/2025 - 11:06","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"50b22fb9-9b80-46da-8f44-c1691ffc14cd","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure3c.csv","description":"\u003Cp\u003EThe temporal variation of the discharge voltage (U), electric current (I) and voltage drop at the resistor (IR) in MGM. The data are given in a form of table where the first column represents time, the second column is the voltage, the third column is the electric current and the fourth is the voltage drop at the resistor (IR).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.3(c)","mimetype":"text\/csv","size":"193.49 KB","created":"Wed, 05\/28\/2025 - 11:09","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"9c4a765e-6c29-422f-88ff-e96965799efb","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure4b.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the electron number density in case of TSM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the number density of electrons at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure4b\u003Cbr \/\u003E\nSize: 1414884\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: n_e [m^-3]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.4(b)","mimetype":"application\/octet-stream","size":"32.39 MB","created":"Wed, 05\/28\/2025 - 11:18","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"f15f8bc0-995a-4cd6-ba0b-811cb1a1f393","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure4c.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the rate of direct ionisation in case of TSM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the rate of direct ionisation at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure4c\u003Cbr \/\u003E\nSize: 491154\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: Rate [m^-3s^-1]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.4(c)","mimetype":"application\/octet-stream","size":"11.24 MB","created":"Wed, 05\/28\/2025 - 11:20","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"5f75d7f3-d3e1-4f14-a466-fcdc6d0a65f7","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure4d.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the rate of stepwise ionisation in case of TSM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the rate of stepwise ionisation at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure4d\u003Cbr \/\u003E\nSize: 491154\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: Rate [m^-3s^-1]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.4(d)","mimetype":"application\/octet-stream","size":"11.24 MB","created":"Wed, 05\/28\/2025 - 11:22","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"0d3fbc86-f429-45b2-b4e4-5dafdc8a0e2e","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure5a.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and electric field along the discharge axis at time 134.220 microseconds during the TSM. The table contains the axial position in the first column, and number densities of the particles and the electric field in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: z [m]\u003Cbr \/\u003E\ncolumn 2: [e] [m^-3] at 134.220 microseconds\u003Cbr \/\u003E\ncolumn 3: [Ar_2^+] [m^-3] at 134.220 microseconds\u003Cbr \/\u003E\ncolumn 4: [Ar^+] [m^-3] at 134.220 microseconds\u003Cbr \/\u003E\ncolumn 5: [Ar_2^*] [m^-3] at 134.220 microseconds\u003Cbr \/\u003E\ncolumn 6: [Ar^*] [m^-3] at 134.220 microseconds\u003Cbr \/\u003E\ncolumn 7: E [kV\/cm] at 134.220 microseconds\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.5(a)","mimetype":"text\/csv","size":"115.72 KB","created":"Wed, 05\/28\/2025 - 11:25","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"6953d659-12c7-4997-b71e-c874c054d569","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure5b.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and electric field along the discharge axis at time 134.316 microseconds during the TSM. The table contains the axial position in the first column, and number densities of the particles and the electric field in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: z [m]\u003Cbr \/\u003E\ncolumn 2: [e] [m^-3] at 134.316 microseconds\u003Cbr \/\u003E\ncolumn 3: [Ar_2^+] [m^-3] at 134.316 microseconds\u003Cbr \/\u003E\ncolumn 4: [Ar^+] [m^-3] at 134.316 microseconds\u003Cbr \/\u003E\ncolumn 5: [Ar_2^*] [m^-3] at 134.316 microseconds\u003Cbr \/\u003E\ncolumn 6: [Ar^*] [m^-3] at 134.316 microseconds\u003Cbr \/\u003E\ncolumn 7: E [kV\/cm] at 134.316 microseconds\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.5(b)","mimetype":"text\/csv","size":"110.46 KB","created":"Wed, 05\/28\/2025 - 11:28","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"085eabde-23d8-4cae-8f80-ba4fdb570779","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure6b.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the electron number density in case of TGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the number density of electrons at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure6b\u003Cbr \/\u003E\nSize: 6116144\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: n_e [m^-3]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.6(b)","mimetype":"application\/octet-stream","size":"139.99 MB","created":"Wed, 05\/28\/2025 - 16:03","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"4322795b-f869-43d6-9a22-fff08db5b2ce","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure6c.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the rate of direct ionisation in case of TGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the rate of direct ionisation at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure6c\u003Cbr \/\u003E\nSize: 6038040\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: Rate [m^-3s^-1]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.6(c)","mimetype":"application\/octet-stream","size":"138.2 MB","created":"Wed, 05\/28\/2025 - 16:07","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"3998472a-fd79-4c94-8c50-17f1334e9943","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure6d.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the rate of stepwise ionisation in case of TGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the rate of stepwise ionisation at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure6d\u003Cbr \/\u003E\nSize: 6038040\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: Rate [m^-3s^-1]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.6(d)","mimetype":"application\/octet-stream","size":"138.2 MB","created":"Wed, 05\/28\/2025 - 16:10","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"3d42b2b6-33f1-48c2-a519-8df866bb4fee","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure7a.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and electric field along the discharge axis at time 51.100 microseconds during the TGM. The table contains the axial position in the first column, and number densities of the particles and the electric field in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: z [m]\u003Cbr \/\u003E\ncolumn 2: [e] [m^-3] at 51.100 microseconds\u003Cbr \/\u003E\ncolumn 3: [Ar_2^+] [m^-3] at 51.100 microseconds\u003Cbr \/\u003E\ncolumn 4: [Ar^+] [m^-3] at 51.100 microseconds\u003Cbr \/\u003E\ncolumn 5: [Ar_2^*] [m^-3] at 51.100 microseconds\u003Cbr \/\u003E\ncolumn 6: [Ar^*] [m^-3] at 51.100 microseconds\u003Cbr \/\u003E\ncolumn 7: E [kV\/cm] at 51.100 microseconds\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.7(a)","mimetype":"text\/csv","size":"113.74 KB","created":"Wed, 05\/28\/2025 - 16:12","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"819bcabc-0e64-4dcc-ae09-a139fbaa23d7","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure7b.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and electric field along the discharge axis at time 51.393 microseconds during the TGM. The table contains the axial position in the first column, and number densities of the particles and the electric field in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: z [m]\u003Cbr \/\u003E\ncolumn 2: [e] [m^-3] at 51.393 microseconds\u003Cbr \/\u003E\ncolumn 3: [Ar_2^+] [m^-3] at 51.393 microseconds\u003Cbr \/\u003E\ncolumn 4: [Ar^+] [m^-3] at 51.393 microseconds\u003Cbr \/\u003E\ncolumn 5: [Ar_2^*] [m^-3] at 51.393 microseconds\u003Cbr \/\u003E\ncolumn 6: [Ar^*] [m^-3] at 51.393 microseconds\u003Cbr \/\u003E\ncolumn 7: E [kV\/cm] at 51.393 microseconds\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.7(b)","mimetype":"text\/csv","size":"113.29 KB","created":"Wed, 05\/28\/2025 - 16:13","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"a6d8c68c-75ab-467a-9bd9-f90e1be43b27","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure8.csv","description":"\u003Cp\u003ETemporal evolution of the number density of electrons and Ar_2^+ ions and the mean electron energy during the establishment of the MGM. The data are stored in a table where the first column is the axial position, the second column is spatially averaged number density of electrons, the third is electron number density at 0.1 mm, the fourth electron number density at 0.75 mm, the fifth spatially averaged number density of Ar_2^+, ions, the sixth their value at 0.1 mm, the seventh their value at 0.75mm, the eight spatially averaged mean electron energy and ninth and tenth are mean electron energy at 0.1 mm and 0.75 mm, respectively.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: t [s]\u003Cbr \/\u003E\ncolumn 2: n_e_mean [m^-3]\u003Cbr \/\u003E\ncolumn 3: n_e@0.1mm [m^-3]\u003Cbr \/\u003E\ncolumn 4: n_e@0.75mm [m^-3]\u003Cbr \/\u003E\ncolumn 5: Ar_2^+_mean [m^-3]\u003Cbr \/\u003E\ncolumn 6: Ar_2^+@0.1mm [m^-3]\u003Cbr \/\u003E\ncolumn 7: Ar_2^+@0.75mm [m^-3]\u003Cbr \/\u003E\ncolumn 8: u_e_mean [eV]\u003Cbr \/\u003E\ncolumn 9: u_e@0.1mm [eV]\u003Cbr \/\u003E\ncolumn 10: u_e@0.75mm [eV]\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.8","mimetype":"text\/csv","size":"6.94 KB","created":"Wed, 05\/28\/2025 - 16:15","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"b6243f03-c88b-4aec-a915-1afd20906234","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure9a.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the number density of Ar_2^* in MGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the number density of Ar_2^* at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure4b\u003Cbr \/\u003E\nSize: 6009502\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: n_Ar_2^* [m^-3]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.9(a)","mimetype":"application\/octet-stream","size":"137.55 MB","created":"Wed, 05\/28\/2025 - 16:18","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"f99fc02d-a224-434e-935b-35c83b17b7d9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure9b_and_c.csv","description":"\u003Cp\u003ETemporal evolution of the electron production rates during the establishment of the MGM. The data are stored in a table where the first column is the time, the second column is the rate of direct ionisation, the third is rate of ionisation of excited atom, the fourth the rate of ionisation of excimers and the fifth is the rate of chemo-ionisation.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: t [s]\u003Cbr \/\u003E\ncolumn 2: direct ionisation [m^-3s^-1]\u003Cbr \/\u003E\ncolumn 3: Ar^* ionisation  [m^-3s^-1]\u003Cbr \/\u003E\ncolumn 4: Ar_2^* ionisation [m^-3s^-1]\u003Cbr \/\u003E\ncolumn 5: chemo-ionisation [m^-3s^-1]\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.9(b,c)","mimetype":"text\/csv","size":"220.36 KB","created":"Wed, 05\/28\/2025 - 16:21","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"1f23d409-bd11-4401-95e0-617cecf98d63","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure10b.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the electron number density in case of MGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the number density of electrons at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure10b\u003Cbr \/\u003E\nSize: 315420\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: n_e [m^-3]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.10(b)","mimetype":"application\/octet-stream","size":"7.22 MB","created":"Wed, 05\/28\/2025 - 16:23","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"223e56d7-98d4-44ef-bb2d-0c08b75d53ec","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure10c.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the rate of direct ionisation in case of MGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the direct ionisation at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure10c\u003Cbr \/\u003E\nSize: 315420\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: Rate [m^-3s^-1]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.10(c)","mimetype":"application\/octet-stream","size":"7.22 MB","created":"Wed, 05\/28\/2025 - 16:24","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"77db7855-1ddd-4230-8f9a-e805a7be1338","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure10d.h5","description":"\u003Cp\u003EThe spatiotemporal evolution of the rate of stepwise ionisation in case of MGM is provided in this file. Due to the 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 for a given time in the first column all axial positions are varied in the second column, whereas the third column contains the rate of stepwise ionisation at the given time and position.\u003C\/p\u003E\n\u003Cp\u003EDataset: Figure10d\u003Cbr \/\u003E\nSize: 315420\u003Cbr \/\u003E\nStructured array: column 1: t [s]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 2: z [m]: H5T_IEEE_F64LE (double)\u003Cbr \/\u003E\ncolumn 3: Rate [m^-3s^-1]: H5T_IEEE_F64LE (double)\u003C\/p\u003E\n","format":"hdf5","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.10(d)","mimetype":"application\/octet-stream","size":"7.22 MB","created":"Wed, 05\/28\/2025 - 16:26","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"03cae009-bccf-4ed4-8685-e9da546fc461","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure11a.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and electric field along the discharge axis at time 148.050 microseconds during the MGM. The table contains the axial position in the first column, and number densities of the particles and the electric field in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: z [m]\u003Cbr \/\u003E\ncolumn 2: [e] [m^-3] at 148.050 microseconds\u003Cbr \/\u003E\ncolumn 3: [Ar_2^+] [m^-3] at 148.050 microseconds\u003Cbr \/\u003E\ncolumn 4: [Ar^+] [m^-3] at 148.050 microseconds\u003Cbr \/\u003E\ncolumn 5: [Ar_2^*] [m^-3] at 148.050 microseconds\u003Cbr \/\u003E\ncolumn 6: [Ar^*] [m^-3] at 148.050 microseconds\u003Cbr \/\u003E\ncolumn 7: E [kV\/cm] at 148.050 microseconds\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.11(a)","mimetype":"text\/csv","size":"116.68 KB","created":"Wed, 05\/28\/2025 - 16:27","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"2cf9d6a2-4b2f-4650-bc01-2eaaf2ead350","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure11b.csv","description":"\u003Cp\u003ESpatial profiles of the number densities of all included particle species, and electric field along the discharge axis at time 150.800 microseconds during the MGM. The table contains the axial position in the first column, and number densities of the particles and the electric field in the following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: z [m]\u003Cbr \/\u003E\ncolumn 2: [e] [m^-3] at 150.800 microseconds\u003Cbr \/\u003E\ncolumn 3: [Ar_2^+] [m^-3] at 150.800 microseconds\u003Cbr \/\u003E\ncolumn 4: [Ar^+] [m^-3] at 150.800 microseconds\u003Cbr \/\u003E\ncolumn 5: [Ar_2^*] [m^-3] at 150.800 microseconds\u003Cbr \/\u003E\ncolumn 6: [Ar^*] [m^-3] at 150.800 microseconds\u003Cbr \/\u003E\ncolumn 7: E [kV\/cm] at 150.800 microseconds\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.11(b)","mimetype":"text\/csv","size":"116.21 KB","created":"Wed, 05\/28\/2025 - 16:29","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"607a6d2d-9717-41ee-b04c-c5c47d0d8b72","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure12.csv","description":"\u003Cp\u003ESelf-pulsing frequency, breakdown voltage magnitude and current peak value for different resistances. To avoid repeating data, all the quantities shown in Figure 12 (a and b) are presented in a single table, which contains the resistance in the first column and self-pulsing frequency, breakdown voltage magnitudes, current peak values and modes it following columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: R [10^6 ohm] resistance\u003Cbr \/\u003E\ncolumn 2: f [kHz] self-pulsing frequency\u003Cbr \/\u003E\ncolumn 3: U_d^b [kV] breakdown voltage magnitude\u003Cbr \/\u003E\ncolumn 4: I_d^b [mA] current peak value\u003Cbr \/\u003E\ncolumn 5: Mode\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.12","mimetype":"text\/csv","size":"224 bytes","created":"Wed, 05\/28\/2025 - 16:33","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"},{"id":"bd7ae585-d114-46fc-b0a5-41f237853b59","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node893_figure13.csv","description":"\u003Cp\u003ESelf-pulsing frequency and current peak value for different applied voltages. The table contains the applied voltage in the first column, and current peak values, the self-pulsing frequency and modes in the subsequent columns.\u003C\/p\u003E\n\u003Cp\u003Ecolumn 1: U_0 [kV] applied voltage\u003Cbr \/\u003E\ncolumn 2: I_d^b [mA] current peak value\u003Cbr \/\u003E\ncolumn 3: f [kHz] self-pulsing frequency\u003Cbr \/\u003E\ncolumn 4: Mode\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 07\/15\/2025 - 15:56","name":"Discharge modes of self-pulsing discharges in argon at atmospheric pressure - Fig.13","mimetype":"text\/csv","size":"121 bytes","created":"Wed, 05\/28\/2025 - 16:36","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 07\/15\/2025 - 15:56"}],"tags":[{"id":"ae33de4f-a3ce-469a-9d84-04e5300a5234","vocabulary_id":"2","name":"Self-pulsing"},{"id":"95452d90-ed0c-41cc-a020-93759a51d243","vocabulary_id":"2","name":"fluid modelling"},{"id":"50a392b1-02f5-4bec-b2d5-715f7f841a6e","vocabulary_id":"2","name":"spark discharge"},{"id":"a273a978-d4ca-4b94-b053-3a9ee5adbd23","vocabulary_id":"2","name":"glow 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"}]}]}