MATLAB is needed to access the data, and ".m" is used to plot the figure.
257 files in this archive
- Fig9/
- Fig9/9a_wall_gamma0_gamma1_Kuh21_3kv200ns.jpg
- Fig9/9a_wall_gamma0_gamma1_Kuh21_3kv200ns.pdf
- Fig9/9b_wall_gamma1e_3_gamma7e_3_Kuh21_3kv200ns.jpg
- Fig9/9b_wall_gamma1e_3_gamma7e_3_Kuh21_3kv200ns.pdf
- Fig9/Fig9a_make_plot_paper7_Nratio_gamma0_gamma1.m
- Fig9/Fig9b_make_plot_paper7_Nratio_gamma1e_3_gamma7e_3.m
- Fig9/initialization.m
- Fig9/parameters_pulsed.m
- Fig9/RouteRemark.txt
- Fig9/0_data_A1_A2/
- Fig9/0_data_A1_A2/importfile.m
- Fig9/0_data_A1_A2/importpower.m
- Fig9/0_data_A1_A2/import_a2data.m
- Fig9/0_data_A1_A2/neededParameterForBenchmarking.mat
- Fig9/0_data_A1_A2/power.txt
- Fig9/0_data_A1_A2/SimParameters.m
- Fig9/0_data_A1_A2/SimParametersP.m
- Fig9/0_data_A1_A2/200228_2/
- Fig9/0_data_A1_A2/200228_2/time_evolution_current
- Fig9/0_data_A1_A2/200228_2/time_evolution_energy
- Fig9/0_data_A1_A2/200228_2/time_evolution_num_quanta
- Fig9/0_data_A1_A2/200228_2/time_evolution_T01
- Fig9/0_data_A1_A2/200228_2/time_evolution_T1U
- Fig9/0_data_A1_A2/200228_2/time_evolution_Trot
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=0
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=1
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=2
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=3
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=4
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=5
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=6
- Fig9/0_data_A1_A2/200228_2/time_evolution_v=7
- Fig9/0_data_A1_A2/200228_2/time_evolution_vib_energy
- Fig9/0_data_A1_A2/200228_2/time_evolution_voltage
- Fig9/0_data_A1_A2/210504/
- Fig9/0_data_A1_A2/210504/importfile1.m
- Fig9/0_data_A1_A2/210504/Nv_3kV_200ns.csv
- Fig9/0_data_A1_A2/210504/Nv_3kV_250ns.csv
- Fig9/0_data_A1_A2/210504/Nv_4kV_200ns.csv
- Fig9/0_data_A1_A2/210504/Screenshot from 2021-05-07 17-38-57.png
- Fig9/0_data_A1_A2/220628_Kuh21_2/
- Fig9/0_data_A1_A2/220628_Kuh21_2/get_n_Te.m
- Fig9/0_data_A1_A2/220628_Kuh21_2/ne_1_3kv200ns.csv
- Fig9/0_data_A1_A2/220628_Kuh21_2/ne_2_3kv250ns.csv
- Fig9/0_data_A1_A2/220628_Kuh21_2/ne_3_4kv200ns.csv
- Fig9/0_data_A1_A2/220628_Kuh21_2/Screenshot from 2022-06-28 12-16-07.png
- Fig9/0_data_A1_A2/220628_Kuh21_2withAfterglow/
- Fig9/0_data_A1_A2/220628_Kuh21_2withAfterglow/get_n_Te.m
- Fig9/0_data_A1_A2/220628_Kuh21_2withAfterglow/ne_1_3kv200ns.csv
- Fig9/0_data_A1_A2/220628_Kuh21_2withAfterglow/ne_2_3kv250ns.csv
- Fig9/0_data_A1_A2/220628_Kuh21_2withAfterglow/ne_3_4kv200ns.csv
- Fig9/0_data_A1_A2/220628_Kuh21_2withAfterglow/Screenshot from 2022-06-28 12-16-07.png
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_200ns.zip
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_250ns.zip
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/4kV_200ns.zip
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/importfile2.m
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/RUB Webmail __ Fwd_ Densities.pdf
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_200ns/
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_200ns/3kV_200ns.csv
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_200ns/qbranch_population_densities.csv
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_250ns/
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_250ns/3kV_250ns.csv
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/3kV_250ns/qbranch_population_densities.csv
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/4kV_200ns/
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/4kV_200ns/4kV_200ns.csv
- Fig9/0_data_A1_A2/240725_R1C8_N2v_ErrorBar/4kV_200ns/qbranch_population_densities.csv
- Fig9/InputFolder/
- Fig9/InputFolder/elasticCollisions.csv
- Fig9/InputFolder/elasticCollisions_previous.csv
- Fig9/InputFolder/initialValues_pulsed.csv
- Fig9/InputFolder/InitialValue_change.m
- Fig9/InputFolder/InputFile_pulsed.txt
- Fig9/InputFolder/ionWallReactions.csv
- Fig9/InputFolder/lokinames.csv
- Fig9/InputFolder/lokinames_comment.csv
- Fig9/InputFolder/neutralWallReactions.csv
- Fig9/InputFolder/reactions.csv
- Fig9/InputFolder/reactions_previous.csv
- Fig9/InputFolder/species.csv
- Fig9/InputFolder/speciesProperties.csv
- Fig9/InputFolder/reactionPreparation/
- Fig9/InputFolder/reactionPreparation/backwards/
- Fig9/InputFolder/reactionPreparation/backwards/ev-temp.csv
- Fig9/InputFolder/reactionPreparation/backwards/neededParameterForBenchmarking.mat
- Fig9/InputFolder/reactionPreparation/backwards/vv_N2N2inv.csv
- Fig9/InputFolder/reactionPreparation/backwards/vv_z_F.asv
- Fig9/InputFolder/reactionPreparation/backwards/vv_z_F.m
- Fig9/InputFolder/reactionPreparation/forward/
- Fig9/InputFolder/reactionPreparation/forward/ev-temp.csv
- Fig9/InputFolder/reactionPreparation/forward/vv_N2N2.csv
- Fig9/InputFolder/reactionPreparation/forward/vv_z_F.m
- Fig9/Output/
- Fig9/Output/N2Pulsed/
- Fig9/Output_gamma0/
- Fig9/Output_gamma0/N2Pulsed/
- Fig9/Output_gamma0/N2Pulsed/Pulseoff_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseoff_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseoff_3.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseoff_4.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseoff_5.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseoff_6.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_1_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_1_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_1_3.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_2_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_2_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_2_3.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_3_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_3_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_3_3.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_4_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_4_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_4_3.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_5_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_5_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_5_3.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_6_1.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_6_2.mat
- Fig9/Output_gamma0/N2Pulsed/Pulseon_6_3.mat
- Fig9/Output_gamma0/N2Pulsed/results.mat
- Fig9/Output_gamma1/
- Fig9/Output_gamma1/N2Pulsed/
- Fig9/Output_gamma1/N2Pulsed/Pulseoff_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseoff_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseoff_3.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseoff_4.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseoff_5.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseoff_6.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_1_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_1_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_1_3.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_2_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_2_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_2_3.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_3_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_3_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_3_3.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_4_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_4_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_4_3.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_5_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_5_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_5_3.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_6_1.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_6_2.mat
- Fig9/Output_gamma1/N2Pulsed/Pulseon_6_3.mat
- Fig9/Output_gamma1/N2Pulsed/results.mat
- Fig9/Output_gamma1e_3/
- Fig9/Output_gamma1e_3/N2Pulsed/
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseoff_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseoff_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseoff_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseoff_4.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseoff_5.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseoff_6.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_1_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_1_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_1_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_2_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_2_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_2_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_3_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_3_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_3_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_4_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_4_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_4_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_5_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_5_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_5_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_6_1.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_6_2.mat
- Fig9/Output_gamma1e_3/N2Pulsed/Pulseon_6_3.mat
- Fig9/Output_gamma1e_3/N2Pulsed/results.mat
- Fig9/Output_gamma3e_3/
- Fig9/Output_gamma3e_3/N2Pulsed/
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseoff_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseoff_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseoff_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseoff_4.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseoff_5.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseoff_6.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_1_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_1_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_1_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_2_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_2_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_2_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_3_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_3_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_3_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_4_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_4_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_4_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_5_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_5_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_5_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_6_1.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_6_2.mat
- Fig9/Output_gamma3e_3/N2Pulsed/Pulseon_6_3.mat
- Fig9/Output_gamma3e_3/N2Pulsed/results.mat
- Fig9/Output_gamma7e_3/
- Fig9/Output_gamma7e_3/N2Pulsed/
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseoff_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseoff_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseoff_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseoff_4.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseoff_5.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseoff_6.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_1_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_1_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_1_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_2_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_2_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_2_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_3_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_3_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_3_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_4_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_4_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_4_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_5_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_5_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_5_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_6_1.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_6_2.mat
- Fig9/Output_gamma7e_3/N2Pulsed/Pulseon_6_3.mat
- Fig9/Output_gamma7e_3/N2Pulsed/results.mat
- Fig9/Output_ref/
- Fig9/Output_ref/N2Pulsed/
- Fig9/Output_ref/N2Pulsed/Pulseoff_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseoff_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseoff_3.mat
- Fig9/Output_ref/N2Pulsed/Pulseoff_4.mat
- Fig9/Output_ref/N2Pulsed/Pulseoff_5.mat
- Fig9/Output_ref/N2Pulsed/Pulseoff_6.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_1_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_1_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_1_3.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_2_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_2_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_2_3.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_3_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_3_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_3_3.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_4_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_4_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_4_3.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_5_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_5_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_5_3.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_6_1.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_6_2.mat
- Fig9/Output_ref/N2Pulsed/Pulseon_6_3.mat
- Fig9/Output_ref/N2Pulsed/results.mat