31. Raw data and background rates    Appendix

In this appendix we find a few more figures and numbers about the background rates and a comparison to the raw data rates. Fig. 1 shows the raw data rate of the full center chip of the entire CAST data taking campaign in the same units as used for the normal background rate plots. The background increases towards low energies, but a hump is visible in the \(\SIrange{2}{3}{keV}\) range, matching the expected energies for muon tracks. The rates are roughly four orders of magnitude larger than the best achieved background rates.

all_cast_data_rate_crAll_chip_3_log.svg
Figure 1: Figure 190: All CAST data of the entire center chip without any classifier or other cuts. Uses the same units as all background plots for easier comparison.

Further, in sec. 31.1 we find background rates not only for the \goldArea region, but for the entire center chip. Both to compare with fig. 1 as well as to get a better idea of the efficiency of the vetoes.

31.1. Background rates over full chip

Fig. 2 shows the effect of the different vetoes over the entire chip using the \lnL method at \(\SI{80}{\%}\) software efficiency as a base. It better highlights the efficiency of some vetoes, for example the FADC veto is more effective over the entire chip, than in the center \goldArea region alone (compare with fig. 71). Of course, the septem and line vetoes are even more efficient over the entire chip, as expected and previously seen in the form of the background suppression plots (for example fig. #fig:background:background_suppression_comparison).

Fig. 3 shows how the different software efficiencies affect the background rate comparing different \lnL and MLP efficiencies including all vetoes.

Finally, tab. 30 shows the mean background rates over the entire chip for all considered \lnL and MLP veto setups in the energy range \(\SIrange{0.2}{8}{keV}\). It is the equivalent of tab. 24 for the full chip.

background_rate_crAll_lnL80.svg
Figure 2: Figure 191: Background rate over the entire center chip of all CAST data, comparing the \lnL cut method at \(\SI{80}{\%}\) software efficiency without any vetoes with each veto setup (vetoes are additive again).
background_rate_crAll_all_vetoes_lnL_mlp.svg
Figure 3: Figure 192: Background rate over the entire center chip of all CAST data, comparing the \lnL cut method and the MLP at different software efficiencies including all vetoes.
Table 30: Mean background rates in \(\si{keV^{-1}.cm^{-2}.s^{-1}}\) over the entire chip comparing all different \lnL and MLP setups in an energy range from \(\SIrange{0.2}{8}{keV}\). Due to its efficiency at lower energies, where the majority of background is, the MLP produces the lowest mean rates.
Classifier \(ε_{\text{eff}}\) Scinti FADC Septem Line \(ε_{\text{total}}\) Rate [\(\si{keV^{-1}.cm^{-2}.s^{-1}}\)]
MLP 0.865 true true true true 0.621 \(\num{ 1.73569(3138)e-05}\)
MLP 0.912 true true true true 0.655 \(\num{ 2.26378(3583)e-05}\)
LnL 0.700 true true true true 0.503 \(\num{ 2.54625(3800)e-05}\)
LnL 0.800 true true true true 0.574 \(\num{ 3.30065(4327)e-05}\)
MLP 0.957 true true true true 0.687 \(\num{ 3.55534(4491)e-05}\)
LnL 0.900 true true true true 0.646 \(\num{ 4.51280(5059)e-05}\)
MLP 0.865 true true false true 0.729 \(\num{ 4.90021(5272)e-05}\)
LnL 0.800 true true true false 0.615 \(\num{ 5.48218(5576)e-05}\)
MLP 0.983 true true true true 0.706 \(\num{ 5.79245(5732)e-05}\)
MLP 0.912 true true false true 0.769 \(\num{ 6.25757(5958)e-05}\)
LnL 0.700 true true false true 0.590 \(\num{ 6.59450(6116)e-05}\)
LnL 0.800 true true false true 0.674 \(\num{ 8.42889(6915)e-05}\)
MLP 0.957 true true false true 0.807 \(\num{ 9.12033(7193)e-05}\)
LnL 0.900 true true false true 0.759 \(\num{1.107044(7924)e-04}\)
MLP 0.983 true true false true 0.829 \(\num{1.344765(8734)e-04}\)
MLP 0.865 false false false false 0.865 \(\num{ 3.09861(1326)e-04}\)
LnL 0.700 false false false false 0.700 \(\num{ 3.35726(1380)e-04}\)
LnL 0.800 true true false false 0.784 \(\num{ 3.79510(1467)e-04}\)
MLP 0.912 false false false false 0.912 \(\num{ 3.90043(1487)e-04}\)
LnL 0.800 true false false false 0.800 \(\num{ 4.21893(1547)e-04}\)
LnL 0.800 false false false false 0.800 \(\num{ 4.26918(1556)e-04}\)
MLP 0.957 false false false false 0.957 \(\num{ 5.33187(1739)e-04}\)
LnL 0.900 false false false false 0.900 \(\num{ 5.60453(1783)e-04}\)
MLP 0.983 false false false false 0.983 \(\num{ 7.25588(2029)e-04}\)

31.2. Generate rate without any vetoes over full chip    extended

We will use the same units as for the background rate for easier comparison! i.e. 1e-5 keV⁻¹·cm⁻²·s⁻¹

plotBackgroundRate \
    ~/CastData/data/DataRuns2017_Reco.h5 \
    ~/CastData/data/DataRuns2018_Reco.h5 \
    --names "All" --names "All" \
    --centerChip 3 \
    --title "Raw CAST data rate" \
    --showNumClusters \
    --region crAll \
    --showTotalTime \
    --topMargin 1.5 \
    --energyDset energyFromCharge \
    --energyMin 0.0 \
    --outfile all_cast_data_rate_crAll_chip_3_log.pdf \
    --outpath ~/phd/Figs/CAST_raw_data \
    --useTeX \
    --quiet

31.3. Generate background rates over full chip    extended

  • [ ] Adjust the below to use the interesting input files. The region is already crAll. Just need to remove the files we don't want for different plots.

LnL 80% veto setups:

WRITE_PLOT_CSV=true plotBackgroundRate \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_septem_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_septem_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_line_vQ_0.99.h5 \
    --names "No vetoes" --names "No vetoes" \
    --names "Scinti" --names "Scinti" \
    --names "FADC" --names "FADC" \
    --names "Septem" --names "Septem" \
    --names "All vetoes" --names "All vetoes" \
    --names "Line" --names "Line" \
    --centerChip 3 \
    --title "Background rate from CAST data over entire chip, lnL@80% incl. vetoes" \
    --showNumClusters \
    --showTotalTime \
    --topMargin 1.5 \
    --energyDset energyFromCharge \
    --outfile background_rate_crAll_lnL80.pdf \
    --outpath ~/phd/Figs/background/ \
    --region crAll \
    --useTeX \
    --logPlot \
    --hidePoints --hideErrors \
    --quiet

Comparison of different lnL and MLP setups with all vetoes in place:

WRITE_PLOT_CSV=true plotBackgroundRate \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    --names "lnL@80" --names "lnL@80" \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.7_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.7_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    --names "lnL@70" --names "lnL@70" \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.9_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.9_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    --names "lnL@90" --names "lnL@90" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.85_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.85_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@85" --names "MLP@85" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.9_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.9_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@90" --names "MLP@90" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.95_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.95_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@95" --names "MLP@95" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.98_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.98_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@98" --names "MLP@98" \
    --centerChip 3 \
    --title "Background rate from CAST data over entire chip, all vetoes" \
    --showNumClusters \
    --showTotalTime \
    --topMargin 1.5 \
    --energyDset energyFromCharge \
    --outfile background_rate_crAll_all_vetoes_lnL_mlp.pdf \
    --outpath ~/phd/Figs/background/ \
    --region crAll \
    --energyMin 0.2 \
    --useTeX \
    --logPlot \
    --hidePoints --hideErrors \
    --quiet

31.4. Generate table of background rates for all setups    extended

We use the background rate plotting tool to produce a table of the background rates over the entire chip in an energy range from 0 to 8 keV. Note the --rateTable argument at the end in the massive wall below:

WRITE_PLOT_CSV=true plotBackgroundRate \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_septem_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_septem_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.8_lnL_scinti_fadc_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.8_lnL_scinti_fadc_line_vQ_0.99.h5 \
    --names "LnL80" --names "LnL80" \
    --names "LnL80+Sc" --names "LnL80+Sc" \
    --names "LnL80+F" --names "LnL80+F" \
    --names "LnL80+S" --names "LnL80+S" \
    --names "LnL80+SL" --names "LnL80+SL" \
    --names "LnL80+L" --names "LnL80+L" \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.7_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.7_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.7_lnL_scinti_fadc_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.7_lnL_scinti_fadc_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.7_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.7_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    --names "LnL70" --names "LnL70" \
    --names "LnL70+L" --names "LnL70+L" \
    --names "LnL70+S" --names "LnL70+S" \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.9_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.9_lnL.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.9_lnL_scinti_fadc_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.9_lnL_scinti_fadc_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R2_crAll_sEff_0.9_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    ~/org/resources/lhood_lnL_17_11_23_septem_fixed/lhood_c18_R3_crAll_sEff_0.9_lnL_scinti_fadc_septem_line_vQ_0.99.h5 \
    --names "LnL90" --names "LnL90" \
    --names "LnL90+L" --names "LnL90+L" \
    --names "LnL90+S" --names "LnL90+S" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.85_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.85_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.85_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.85_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.85_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.85_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@85" --names "MLP@85" \
    --names "MLP@85+L" --names "MLP@85+L" \
    --names "MLP@85+S" --names "MLP@85+S" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.9_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.9_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.9_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.9_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.9_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.9_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@9" --names "MLP@9" \
    --names "MLP@9+L" --names "MLP@9+L" \
    --names "MLP@9+S" --names "MLP@9+S" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.95_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.95_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.95_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.95_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.95_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.95_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@95" --names "MLP@95" \
    --names "MLP@95+L" --names "MLP@95+L" \
    --names "MLP@95+S" --names "MLP@95+S" \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.98_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.98_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.98_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.98_scinti_fadc_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R2_crAll_sEff_0.98_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    ~/org/resources/lhood_mlp_17_11_23_adam_tanh30_sigmoid_mse_82k/lhood_c18_R3_crAll_sEff_0.98_scinti_fadc_septem_line_mlp_mlp_tanh_sigmoid_MSE_Adam_30_2checkpoint_epoch_82000_loss_0.0249_acc_0.9662_vQ_0.99.h5 \
    --names "MLP@98" --names "MLP@98" \
    --names "MLP@98+L" --names "MLP@98+L" \
    --names "MLP@98+S" --names "MLP@98+S" \
    --centerChip 3 \
    --title "Background rate from CAST data, incl. scinti, FADC, septem, line veto" \
    --showNumClusters \
    --showTotalTime \
    --topMargin 1.5 \
    --energyDset energyFromCharge \
    --outfile background_rate_crAll_different_veto_cases.pdf \
    --outpath ~/phd/Figs/background/ \
    --region crAll \
    --energyMin 0.2 \
    --logPlot --hidePoints --hideErrors \
    --rateTable ~/phd/resources/background_rate_comparisons_crAll.org \
    --noPlot \
    --quiet
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