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--- imrphenomhm_pe_study [2017/09/18 13:42] – [Creating frame files] chinmay.kalaghatgi@LIGO.ORG
+++ imrphenomhm_pe_study [2017/09/18 14:11] (current) – [PE Runs] chinmay.kalaghatgi@LIGO.ORG
@@ Line 21: / Line 21: @@
   * The two detector network injection (H-L) frames can be found at : __/home/c1549390/work/PhenomHM_pe/frames/HL_Frames__
   * The three detector network injection (H-L-V) frames can be found at: __/home/c1549390/work/PhenomHM_pe/frames/HLV_Frames__
+=== PE Runs ===
+  * In some previous runs, we had noticed that the improvement of PhenomHM vs PhenomD to constrain the distance was increased by ~ 50 % (i.e., the posteriors of PhenomHM were narrower by 50% compared to PhenomD ) for the two detector network and for the HLV configuration, the same value was ~ 40%.
+  * One caveat between those two runs was that for the HL run, the source was placed at a sky-position where the response was the maximum, but for the HLV run the source was at a sky-position where the response was about half of that.
+  * I wanted to check the effect of changing the inclination of the source on the recovery and to check for any biases on the posteriors and to check whether including a third detector would improve the results.
+  * With that in mind, I have started a set of runs for the BAM q4 & q8 non-spinning waveforms for two and three detector configuration, at three different inclinations for each. So it's a total of 24 runs.
+  * I've used the aLIGOzeroDetHighPower and aVIRGO PSD's for the runs.
+  * The base directory for all the run directories is at: __/home/c1549390/work/PhenomHM_pe/runs/18_09_2017/__
+^  Simulation h5 file  ^  Detector configuration  ^  Inclination  ^  Waveform  ^ Date started  ^  Run Directory : basedir + ^  Status  ^  Results page  ^
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HL  |  0 | IMRPhenomD | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_0.0_M80_HL_PhenomD | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HL  |  60 | IMRPhenomD | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_60.0_M80_HL_PhenomD | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HL  |  90 | IMRPhenomD | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_90.0_M80_HL_PhenomD | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HL  |  0 | IMRPhenomHM | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_0.0_M80_HL_PhenomHM | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HL  |  60 | IMRPhenomHM | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_60.0_M80_HL_PhenomHM | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HL  |  90 | IMRPhenomHM | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_90.0_M80_HL_PhenomHM | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HLV  |  0 | IMRPhenomD | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_0.0_M80_HLV_PhenomD | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HLV  |  60 | IMRPhenomD | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_60.0_M80_HLV_PhenomD | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HLV  |  90 | IMRPhenomD | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_90.0_M80_HLV_PhenomD | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HLV  |  0 | IMRPhenomHM | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_0.0_M80_HLV_PhenomHM | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HLV  |  60 | IMRPhenomHM | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_60.0_M80_HLV_PhenomHM | Running | |
+|  q4a0_T_112_448_fix_scale_Lmax_4_Allm.h5 | HLV  |  90 | IMRPhenomHM | 18/09/17 | BAM_q4a0a0_SNR_25_mode_lMax_4_inc_90.0_M80_HLV_PhenomHM | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HL  |  0 | IMRPhenomD | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_0.0_M115_HL_PhenomD | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HL  |  60 | IMRPhenomD | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_60.0_M115_HL_PhenomD | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HL  |  90 | IMRPhenomD | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_90.0_M115_HL_PhenomD | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HL  |  0 | IMRPhenomHM | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_0.0_M115_HL_PhenomHM | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HL  |  60 | IMRPhenomHM | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_60.0_M115_HL_PhenomHM | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HL  |  90 | IMRPhenomHM | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_90.0_M115_HL_PhenomHM | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HLV  |  0 | IMRPhenomD | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_0.0_M115_HLV_PhenomD | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HLV  |  60 | IMRPhenomD | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_60.0_M115_HLV_PhenomD | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HLV  |  90 | IMRPhenomD | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_90.0_M115_HLV_PhenomD | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HLV  |  0 | IMRPhenomHM | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_0.0_M115_HLV_PhenomHM | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HLV  |  60 | IMRPhenomHM | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_60.0_M115_HLV_PhenomHM | Running | |
+|  q8a0a0_T_112_588n768_fix_scale_Lmax_4_Allm.h5 | HLV  |  90 | IMRPhenomHM | 18/09/17 | BAM_q8a0a0_SNR_25_mode_lMax_4_inc_90.0_M115_HLV_PhenomHM | Running | |