{"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":"f1afd462-e16e-4a7c-98aa-f457927e0d5d","name":"extended-reaction-kinetics-model-non-thermal-argon-plasmas-and-its-test-against-experimental","title":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Dataset","author_email":"marjan.stankov@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\u003EModelling results obtained using an extended reaction kinetics model (RKM) suitable for the analysis of weakly ionised, non-thermal argon plasmas with gas temperatures around 300K at sub-atmospheric and atmospheric pressures are presented.  Modelling was performed by means of a time- and space-dependent fluid model for two different dielectric barrier discharge configurations as well as for a micro-scaled atmospheric-pressure plasma jet setup. The results are also compared with measurements, as well as with modelling data obtained by use of a previously established 15-species RKM.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/extended-reaction-kinetics-model-non-thermal-argon-plasmas-and-its-test-against-experimental","state":"Active","log_message":"Update to resource Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 2 (Current)","private":true,"revision_timestamp":"Mon, 02\/20\/2023 - 10:29","metadata_created":"Mon, 07\/04\/2022 - 18:20","metadata_modified":"Mon, 02\/20\/2023 - 10:29","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"88f769d0-2358-4f7c-8501-be1d9afd94d1","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_2_current_0.csv","description":"\u003Cp\u003EThe table contains data showing the temporal evolution of the discharge current obtained by use of the 23-species RKM in the first seven voltage periods at p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz (T = 41.7 \u00b5s).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 2 (Current)","mimetype":"text\/csv","size":"441.27 KB","created":"Wed, 09\/21\/2022 - 11:41","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"214b8546-53c7-4ed6-8885-4d1be33b6828","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_2_electron_density.csv","description":"\u003Cp\u003EThe dataset provides spatiotemporal variation of the electron number density obtained by use of the 23-species RKM in the first seven voltage periods at p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz (T = 41.7 \u00b5s). The first column represents the gap distance values in units of meters, while the first row is a time given in units of seconds. Values for electron number density n_e are given as log(n_e [m^-3]).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 2 (Electron number density)","mimetype":"text\/csv","size":"80.98 MB","created":"Wed, 09\/21\/2022 - 12:01","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"9b9ab33e-da18-4bdc-af25-6831e386c993","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_3_0.csv","description":"\u003Cp\u003EThe data provide the measured and calculated current in the stable periodic state of the discharge. The calculation was performed using the 23-species RKM.  It is important to note that the 15-species RKM could not be applied under the given conditions to analyse the discharge behaviour because the applied voltage was too low to ignite the discharge.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 3","mimetype":"text\/csv","size":"4.45 MB","created":"Wed, 09\/21\/2022 - 15:17","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"258bacb2-f250-48b5-8f87-4faee9365432","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_4_0.csv","description":"\u003Cp\u003EThe table contains data showing the temporal evolution of the spatially averaged mean electron energy u_e and electron number density n_e  obtained by use of the 15-species and 23-species RKM during the first voltage period at p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 4","mimetype":"text\/csv","size":"827.37 KB","created":"Wed, 09\/21\/2022 - 15:25","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"7a9b8803-2831-46f6-bd04-e7761337f15f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_5.csv","description":"\u003Cp\u003EGiven data represent spatial distributions of the electron number density and mean electron energy in the gap at the time t = 1.4 \u00b5s obtained by the 15-species and 23-species RKM  at p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 5","mimetype":"text\/csv","size":"88.35 KB","created":"Wed, 09\/21\/2022 - 15:35","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"1f65bdcb-9fa4-4ee7-94dc-ebb04a0157d7","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_6a.csv","description":"\u003Cp\u003EThe frequencies of electron energy loss used in 15- and 23-species model as a function of the mean electron energy at p = 300 mbar are given by the presented data.  Shown frequencies include electron-impact excitation processes of Ar[1p0 ] to the 1s levels, the 2p levels from 2p10 to 2p5 and the 2p\u0027 levels from 2p4 to 2p1, denoted as red, blue and green lines in the table, respectively.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 6a","mimetype":"text\/csv","size":"12.16 KB","created":"Wed, 09\/21\/2022 - 15:50","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"78476026-c800-43d0-8743-dcd1c63cb180","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_6b.csv","description":"\u003Cp\u003EThe frequencies of electron gain used in 15- and 23-species model as a function of the mean electron energy at p = 300 mbar are given by the presented data. Here electron gain takes into account only the ionisation of ground state argon atoms due to its dominance over the other electron production channels.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 6b","mimetype":"text\/csv","size":"1.84 KB","created":"Wed, 09\/21\/2022 - 15:54","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"e5cf35a3-aec8-4b7f-a96c-f92cee0cccef","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_7_0.csv","description":"\u003Cp\u003EThe data represent periodic behaviour of the measured and calculated Ar[1s5 ] number density,  calculated rates of main gain processes of Ar[1s5 ] and the mean electron energy u_e. Also, rates of main loss processes of Ar[1s5 ] are included. The index i corresponds to the index of the processes in tables 2 and 3 in the manuscript. The data are obtained at p = 300 mbar, U_0 = 1.5 kV and f = 24 kH in the middle of the gap (x = 2.5 mm).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 7","mimetype":"text\/csv","size":"2.04 MB","created":"Wed, 09\/21\/2022 - 16:14","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"70b8b5b0-f156-4da9-af34-c3ff9de0c717","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8a.csv","description":"\u003Cp\u003EGiven data represent a spatiotemporal variation of the measured argon emission at 750.39 nm around breakdown during the first half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz and normalised with respect to their maximum values.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8a","mimetype":"text\/csv","size":"64.01 KB","created":"Wed, 09\/21\/2022 - 16:31","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"85b69c7b-a38e-4b8c-a4c2-6b5d38472db9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8b.csv","description":"\u003Cp\u003EGiven data represent a spatiotemporal variation of the measured argon emission at 750.39 nm around breakdown during the second half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz and normalised with respect to their maximum values.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8b","mimetype":"text\/csv","size":"64.13 KB","created":"Wed, 09\/21\/2022 - 16:32","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"86fcea79-3092-4e3f-84cb-05792c291704","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8c.csv","description":"\u003Cp\u003EGiven data represent spatiotemporal variation of the calculated excitation rate of Ar[2p1 ] atoms in all electron-impact excitation processes around breakdown during the first half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz and normalised with respect to their maximum values.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":" Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8c","mimetype":"text\/csv","size":"2.2 MB","created":"Wed, 09\/21\/2022 - 16:36","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"4bc4689d-94f1-4646-93bc-93d29ba9aefb","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8d.csv","description":"\u003Cp\u003EGiven data represent spatiotemporal variation of the calculated excitation rate of Ar[2p1 ] atoms in all electron-impact excitation processes around breakdown during the second half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz and normalised with respect to their maximum values.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8d","mimetype":"text\/csv","size":"2.24 MB","created":"Wed, 09\/21\/2022 - 16:37","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"f326d62b-9a44-4ed2-b043-b5acf2e52751","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8e.csv","description":"\u003Cp\u003EGiven data represent spatiotemporal variation of the calculated mean electron energy around breakdown during the first half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8e","mimetype":"text\/csv","size":"3.74 MB","created":"Wed, 09\/21\/2022 - 16:40","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"4760d14c-523a-4d97-b133-849b5a37398a","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8f.csv","description":"\u003Cp\u003EGiven data represent spatiotemporal variation of the calculated mean electron energy around breakdown during the second half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8f","mimetype":"text\/csv","size":"3.74 MB","created":"Wed, 09\/21\/2022 - 16:42","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"afb60790-b23c-43eb-af2d-2e583a883326","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8g.csv","description":"\u003Cp\u003EGiven data represent spatiotemporal variation of the calculated electric field around breakdown during the first half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8g","mimetype":"text\/csv","size":"3.68 MB","created":"Wed, 09\/21\/2022 - 16:44","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"c87c70a1-00a0-47ef-8deb-5b0a519900d6","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_8h.csv","description":"\u003Cp\u003EGiven data represent spatiotemporal variation of the calculated electric field around breakdown during the second half-period. The first column contains the values of the distance in the gap given in units of meters, while the first row represents a time given in units of seconds. The data are obtained for p = 300 mbar, U_0 = 1.5 kV and f = 24 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 8h","mimetype":"text\/csv","size":"3.68 MB","created":"Wed, 09\/21\/2022 - 16:48","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"e7334a89-18da-4cae-9b78-c501ec309412","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_9_0.csv","description":"\u003Cp\u003EThe dataset contains the measured (I_experiment_C, I_experiment_R) and calculated (I_15_species_model, I_23_species_model) discharge currents using the 15-species and 23-species RKM in the periodic state of the atmospheric-pressure DBD at U_0 = 4 kV and f = 86.2 kHz. Zero value of the time axis corresponds to t = 84.1 \u00b5s (7.25T).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 9","mimetype":"text\/csv","size":"223.07 KB","created":"Wed, 09\/21\/2022 - 17:03","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"759a98e9-306a-4c2c-8a90-010882cf2635","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_10_0.csv","description":"\u003Cp\u003EThe table contains data for the periodic behaviour of the spatially averaged electron number density (ne_23_species_model, ne_15_species_model) and the discharge current I (I_23_species_model, I_15_species_model) determined by use of the 23- and 15-species RKM. Calculation was made for atmospheric-pressure DBD analysed at U_0 = 4 kV and f = 86.2 kHz.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 10","mimetype":"text\/csv","size":"36.46 KB","created":"Thu, 09\/22\/2022 - 09:04","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"f17f59a3-f025-4486-acda-75da71b1feb8","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_11_current_0.csv","description":"\u003Cp\u003EThe data provides temporal evolution of the discharge current obtained by use of the 23-species RKM in the first seven voltage periods at atmospheric pressure for U_0 = 4 kV and f = 86.2 kHz (T = 41.7 \u00b5s).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 11 (Current)","mimetype":"text\/csv","size":"85.71 KB","created":"Thu, 09\/22\/2022 - 09:13","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"2b9e3f1c-fa56-452a-ac02-053f8e4ecd1e","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_11_electron_density_0.csv","description":"\u003Cp\u003EThe dataset provides spatiotemporal variation of the electron number density obtained by use of the 23-species RKM in the first seven voltage periods at atmospheric pressure for U_0 = 4 kV and f = 86.2 kHz (T = 41.7 \u00b5s). Values for electron number density n_e are given as log(n_e [m^-3]).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 11 (Electron number density)","mimetype":"text\/csv","size":"6.78 MB","created":"Thu, 09\/22\/2022 - 09:24","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"53b85f8c-9175-4465-b2d6-f7ce955a0404","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_12ab_0.csv","description":"\u003Cp\u003EThe data present periodic behaviour of the calculated discharge voltage and current of micro-scaled atmospheric-pressure plasma jet (\u00b5APPJ) at the power of 0.6 and 1.3 W, and the frequency of 27.12 MHz (T = 36.9 ns).  Zero value of the time axis corresponds to t = 88.6 \u00b5s (\u2248 2400T).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 12ab","mimetype":"text\/csv","size":"6.08 KB","created":"Thu, 09\/22\/2022 - 09:39","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"7e96da89-9e5a-406c-ba51-2be1185b9458","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_12c_0.csv","description":"\u003Cp\u003ESpatiotemporal variation of the measured argon emission at 811.53 nm of micro-scaled atmospheric-pressure plasma jet (\u00b5APPJ) at the power of 0.6 W and the frequency of 27.12 MHz (T = 36.9 ns) are given in the table. The first column represents the gap distance values in units of meters, while the first row is a time given in units of seconds. The values of the measured emission are normalised with respect to their maximum values at higher power.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 12c","mimetype":"text\/csv","size":"693.13 KB","created":"Thu, 09\/22\/2022 - 09:55","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"8c4d65d3-ead9-4c51-bf9f-c461bef15df6","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_12d.csv","description":"\u003Cp\u003ESpatiotemporal variation of the measured argon emission at 811.53 nm of micro-scaled atmospheric-pressure plasma jet (\u00b5APPJ) at the power of 1.3 W and the frequency of 27.12 MHz (T = 36.9 ns) are given in the table. The first column represents the gap distance values in units of meters, while the first row is a time given in units of seconds. The values of the measured emission are normalised with respect to their maximum values at higher power.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 12d","mimetype":"text\/csv","size":"627.84 KB","created":"Thu, 09\/22\/2022 - 09:58","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"fa9bca61-439a-49ee-9f6d-d19c78901020","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Fig_12efgh_0.csv","description":"\u003Cp\u003EThe data present spatiotemporal variation of the calculated excitation rate of Ar[2p9 ] atoms in all electron-impact excitation processes and calculated mean electron energy of micro-scaled atmospheric-pressure plasma jet (\u00b5APPJ) at the power of 0.6 and 1.3W and the frequency of 27.12 MHz (T = 36.9 ns). The values of the calculated excitation rates are normalised with respect to their maximum values at higher power. Zero value of the time axis corresponds to t = 88.6 \u00b5s (\u2248 2400T).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - Fig. 12efgh","mimetype":"text\/csv","size":"4.54 MB","created":"Thu, 09\/22\/2022 - 10:16","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"96d4036c-1d71-473c-adf0-87c49fc4ab7c","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/List_of_processes.txt","description":"\u003Cp\u003EThis file contains a list of processes for which the rate coefficients are given in the data set \u0022Rate coefficients for electron-neutral particle collision processes presented in the manuscript\u0022.\u003C\/p\u003E\n","format":"txt","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - list of processes","mimetype":"text\/plain","size":"8.33 KB","created":"Thu, 09\/22\/2022 - 11:35","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"334e2721-ad47-4a7b-b6a5-64f9f1deb9e4","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Rate_coefficients_0.csv","description":"\u003Cp\u003EThe processes presented in the table include 261 electron collision processes with neutral argon species taking into account elastic collisions, excitation, de-excitation and ionisation. The rate coefficients for the processes in this table were determined by solving the steady-state electron Boltzmann equation in multi-term approximation using a generalised version of the method for weakly ionised plasmas presented in the paper of Leyh et al. This method was adapted to include non-conservative electron collisions and the impact of the random motion of gas particles on elastic collision processes. The values for the reduced electric field (E\/N) and gas temperature (T_g ) as well as the cross section data and further atomic data are used as input information. The calculated coefficients are given as a function of the mean electron energy.\u003Cbr \/\u003E\nTo determine the rate coefficients for elastic electron collisions and electron-impact excitation processes the collision cross sections given in the studies of  Zatsarinny et al. were utilised. Cross section data for the electron-impact ionisation of argon in its ground state was taken from the publication of Rapp and Englander-Golden. The analytic formula given by Vriens and Smeets was applied for the determination of the electron-impact ionisation cross sections of excited argon atoms. The same analytic formula was utilised in the case of the ionisation of excited argon molecules, except that the cross section data for the high vibrational levels were taken from the studies of Flannery and McCann. The principle of detailed balance was applied for the determination of the cross sections of electron-impact de-excitation.\u003Cbr \/\u003E\nThe first column in the table represents mean electron energy, while the data in other columns correspond to the rate coefficients listed in the file \u0022List_of_processes.txt\u0022. The last reaction coefficient k_261 corresponds to electron-argon atom elastic collision (N represents the number density of argon atom ground state.).\u003C\/p\u003E\n\u003Cul\u003E\n\u003Cli\u003ELeyh H, Loffhagen D and Winkler R 1998 Comput. Phys. Commun. 113 33\u201348 URL \u003Ca href=\u0022https:\/\/doi.org\/10.1016\/S0010-4655(98)00062-9\u0022\u003Ehttps:\/\/doi.org\/10.1016\/S0010-4655(98)00062-9\u003C\/a\u003E\u003C\/li\u003E\n\u003Cli\u003EZatsarinny O, Wang Y and Bartschat K 2014 Phys. Rev. A 89 022706 BSR database, \u003Ca href=\u0022http:\/\/www.lxcat.net\u0022\u003Ewww.lxcat.net\u003C\/a\u003E, retrieved on May 29, 2018 URL \u003Ca href=\u0022https:\/\/doi.org\/10.1103\/PhysRevA.89.022706\u0022\u003Ehttps:\/\/doi.org\/10.1103\/PhysRevA.89.022706\u003C\/a\u003E\u003C\/li\u003E\n\u003Cli\u003EZatsarinny O, Wang Y and Bartschat K 2014 Phys. Rev. A 89 022706 Private communication of O. Zatsarinny and K. Bartschat, June 6, 2018 URL \u003Ca href=\u0022https:\/\/doi.org\/10.1103\/PhysRevA.89.022706\u0022\u003Ehttps:\/\/doi.org\/10.1103\/PhysRevA.89.022706\u003C\/a\u003E\u003C\/li\u003E\n\u003Cli\u003ERapp D and Englander-Golden P 1965 J. Chem. Phys. 43 1464\u20131479 URL \u003Ca href=\u0022https:\/\/doi.org\/10.1063\/1.1696957\u0022\u003Ehttps:\/\/doi.org\/10.1063\/1.1696957\u003C\/a\u003E\u003C\/li\u003E\n\u003Cli\u003EFlannery M R and McCann K J 1980 Cross sections for ionization of rare gas excimers by electron impact and atomic and molecular processes in excimer laser technical Report AFWAL-TR-80-2015 Georgia Institute of Technology Atlanta, Georgia\u003C\/li\u003E\n\u003C\/ul\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - rate coefficients for electron-neutral particle collision processes ","mimetype":"text\/csv","size":"874.23 KB","created":"Thu, 09\/22\/2022 - 11:28","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"},{"id":"4d51e1a7-15ff-427c-9581-642b72cece75","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node585_Transport_coefficients_0.csv","description":"\u003Cp\u003EThe presented table contains transport coefficients for electrons determined in the same way as the rate coefficients by solving their steady-state Boltzmann equation in multi-term approximation.  The dissipation frequencies of the momentum (Ni) and energy (Ni_energy) flux, as well as the transport coefficients (Xi0, Xi2, Xi0_energy, Xi2_energy), are given as a function of mean electron energy u_mean.  Transport coefficients for ions are given as a function of reduced electric field E\/N .  N represents the number density of argon atom ground state.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 02\/20\/2023 - 10:29","name":"Extended reaction kinetics model for non-thermal argon plasmas and its test against experimental data - electron and ions transport coefficients","mimetype":"text\/csv","size":"25.17 KB","created":"Thu, 09\/22\/2022 - 12:12","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 02\/20\/2023 - 10:29"}],"tags":[{"id":"0f896bf1-4b70-4087-90c3-86d89112b1aa","vocabulary_id":"2","name":"plasma modelling\/simulation"},{"id":"5b5baf77-2e9b-403a-a397-347ed43bfc1f","vocabulary_id":"2","name":"reaction kinetic model"}],"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"}]}]}