IMRPhenomHM PE Study : Aug 2017 onwards

This wiki page is created to note all the motivations for performing specific runs, links to the result pages and codes. The main motivation behind this study is to assess the reliability of IMRPhenomHM waveform to recover physical parameters from injected NR waveforms in zero-noise. We inject NR waveforms in zero-noise so as to suppress all errors from noise contributions to the data.

Choosing the sky position

Creating frame files

PE Runs

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