{"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":"e5bf1955-7ce5-4141-9a78-4d5cfc9b2edf","name":"spatial-density-distribution-h2o2-effluent-cost-jet-and-kinpen-sci-operated-humidified","title":"The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci operated with a humidified helium feed gas - dataset","author":"DO NOT USE","author_email":"levin.kroes@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\u003EThis work serves to highlight the difference of the distinct spatial distribution of H2O2 (hydrogen peroxide) in the effluent of the kINPen-sci plasma jet and the COST reference microplasma jet (COST Jet) operated with humidified helium. For this purpose, the density of H2O2 has been measured spatially resolved using cavity-enhanced absorption spectroscopy employing continuous wave cavity ring-down spectroscopy (cw-CRDS) with a tunable mid-infrared laser. The average number density of H2O2 in the effluent of the kINPen-sci plasma jet is a factor of two higher than in the effluent of the COST Jet. The distribution of H2O2 in the COST-Jet effluent is initially highly uniform and suggests negligible mixing of H2O2 with the ambient air up to 15 mm from the jet nozzle, although it is rapidly diluted at further distances. In the case of the kINPen-sci plasma jet, the number density of H2O2 has a more pronounced radial distribution close to the nozzle, while the mixing with the ambient air is more gradual at further distances from the nozzle.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/spatial-density-distribution-h2o2-effluent-cost-jet-and-kinpen-sci-operated-humidified","state":"Active","log_message":"Update to resource The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci - Fig. 4(a)_data","private":true,"revision_timestamp":"Wed, 10\/25\/2023 - 15:26","metadata_created":"Wed, 10\/11\/2023 - 21:37","metadata_modified":"Wed, 10\/25\/2023 - 15:26","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"8df7380a-b68c-4976-8635-f4ed2349364d","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node784_Fig3.csv","description":"\u003Cp\u003EMeasured cavity loss as a function of wavenumbers as well as the data of model fit to determine the line-of-sight integrated H2O2 density, the pressure broadening coefficient as well as the linear background \u2013 see Fig. 3 in the publication.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 10\/25\/2023 - 15:21","name":"The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci - Fig. 3","mimetype":"text\/csv","size":"264.71 KB","created":"Wed, 10\/25\/2023 - 00:11","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 10\/25\/2023 - 15:21"},{"id":"277e6880-313b-4d70-b7b6-2d5cfaa0a007","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node784_Fig4%28a%29_data.csv","description":"\u003Cp\u003EMeasured normalised line-of-sight integrated absorbance as a function of wavenumber for the kINPen-sci plasma jet between two different distances from the nozzle, at 6 mm and 33 mm. The different shapes illustrate the effect of line broadening \u2013 see Fig 4 in the publication.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 10\/25\/2023 - 15:21","name":"The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci - Fig. 4(a)_data","mimetype":"text\/csv","size":"2.02 KB","created":"Wed, 10\/25\/2023 - 14:17","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 10\/25\/2023 - 15:21"},{"id":"189a315d-e35e-4ebf-9e94-26ea6fd4c3e9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node784_Fig4%28a%29_fit.csv","description":"\u003Cp\u003EModel fit of the line-of-sight integrated absorbance as a function of wavenumber for the kINPen-sci plasma jet between two different distances from the nozzle, at 6 mm and 33 mm. The different shapes illustrate the effect of line broadening \u2013 see Fig 4 in the publication.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 10\/25\/2023 - 15:21","name":"The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci - Fig. 4(a)_fit","mimetype":"text\/csv","size":"312.62 KB","created":"Wed, 10\/25\/2023 - 14:34","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 10\/25\/2023 - 15:21"},{"id":"9ab0db59-5057-43f0-928b-615a145b26ee","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node784_Fig4%28b%29_data.csv","description":"\u003Cp\u003EMeasured normalised line-of-sight integrated absorbance as a function of wavenumber for the COST-Jet between two different distances from the nozzle, at 3 mm and 25 mm. The different shapes illustrate the effect of line broadening \u2013 see Fig 4 in the publication.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 10\/25\/2023 - 15:21","name":"The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci - Fig. 4(b)_data","mimetype":"text\/csv","size":"2.01 KB","created":"Wed, 10\/25\/2023 - 14:37","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 10\/25\/2023 - 15:21"},{"id":"636acf3c-980f-4acb-b8dc-aac9b28741c4","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node784_Fig4%28b%29_fit.csv","description":"\u003Cp\u003EModel fit of the line-of-sight integrated absorbance as a function of wavenumber for the kINPen-sci plasma jet between two different distances from the nozzle, at 3 mm and 25 mm. The different shapes illustrate the effect of line broadening \u2013 see Fig 4 in the publication.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 10\/25\/2023 - 15:21","name":"The spatial density distribution of H2O2 in the effluent of the COST-Jet and the kINPen-sci - Fig. 4(b)_fit","mimetype":"text\/csv","size":"312.62 KB","created":"Wed, 10\/25\/2023 - 14:39","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 10\/25\/2023 - 15:21"},{"id":"628314b7-ee30-4fb3-abcb-a6223fb2dc48","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node784_Fig5.csv","description":"\u003Cp\u003EResults of the pressure broadening coefficient, determined from the model fit of cavity loss spectra, as a function of the axial distance from the nozzle, for the kINPen-sci plasma jet and the COST-Jet, respectively \u2013 see Fig. 5 in the publication.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 10\/25\/2023 - 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