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diff --git a/_c_a_d_mesh_8hh_source.html b/_c_a_d_mesh_8hh_source.html index c6f074ca00..0f56bfc255 100644 --- a/_c_a_d_mesh_8hh_source.html +++ b/_c_a_d_mesh_8hh_source.html @@ -3080,7 +3080,7 @@ diff --git a/_o_m_sim_8cc.html b/_o_m_sim_8cc.html index 6709c7fa87..aee44a385d 100644 --- a/_o_m_sim_8cc.html +++ b/_o_m_sim_8cc.html @@ -134,7 +134,7 @@ diff --git a/_o_m_sim_8hh.html b/_o_m_sim_8hh.html index f98a288cc0..9ad03ac697 100644 --- a/_o_m_sim_8hh.html +++ b/_o_m_sim_8hh.html @@ -151,7 +151,7 @@ diff --git a/_o_m_sim_8hh_source.html b/_o_m_sim_8hh_source.html index f711b671b7..1bce03e100 100644 --- a/_o_m_sim_8hh_source.html +++ b/_o_m_sim_8hh_source.html @@ -200,7 +200,7 @@ diff --git a/_o_m_sim__effective__area_8cc.html b/_o_m_sim__effective__area_8cc.html index 811976b128..81c1d1dbb5 100644 --- a/_o_m_sim__effective__area_8cc.html +++ b/_o_m_sim__effective__area_8cc.html @@ -190,7 +190,7 @@

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diff --git a/_o_m_sim__supernova_8cc.html b/_o_m_sim__supernova_8cc.html index ff1f69dc60..555e4be575 100644 --- a/_o_m_sim__supernova_8cc.html +++ b/_o_m_sim__supernova_8cc.html @@ -230,7 +230,7 @@

  • supernova
  • OMSim_supernova.cc
    • -
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    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/_o_m_sim_angular_scan_8cc.html b/_o_m_sim_angular_scan_8cc.html index cc55779078..9c56742e3c 100644 --- a/_o_m_sim_angular_scan_8cc.html +++ b/_o_m_sim_angular_scan_8cc.html @@ -129,7 +129,7 @@ diff --git a/_o_m_sim_angular_scan_8hh.html b/_o_m_sim_angular_scan_8hh.html index a9187f310e..62aee0fd13 100644 --- a/_o_m_sim_angular_scan_8hh.html +++ b/_o_m_sim_angular_scan_8hh.html @@ -149,7 +149,7 @@ diff --git a/_o_m_sim_angular_scan_8hh_source.html b/_o_m_sim_angular_scan_8hh_source.html index e2c2039f93..4ff4e517b6 100644 --- a/_o_m_sim_angular_scan_8hh_source.html +++ b/_o_m_sim_angular_scan_8hh_source.html @@ -163,7 +163,7 @@ diff --git a/_o_m_sim_command_args_table_8hh.html b/_o_m_sim_command_args_table_8hh.html index 563652fcc6..5072c4cd8d 100644 --- a/_o_m_sim_command_args_table_8hh.html +++ b/_o_m_sim_command_args_table_8hh.html @@ -196,7 +196,7 @@

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diff --git a/_o_m_sim_hit_manager_8hh.html b/_o_m_sim_hit_manager_8hh.html index cae83a36da..4879cdea76 100644 --- a/_o_m_sim_hit_manager_8hh.html +++ b/_o_m_sim_hit_manager_8hh.html @@ -154,7 +154,7 @@ diff --git a/_o_m_sim_hit_manager_8hh_source.html b/_o_m_sim_hit_manager_8hh_source.html index 481105d660..d868fb2503 100644 --- a/_o_m_sim_hit_manager_8hh_source.html +++ b/_o_m_sim_hit_manager_8hh_source.html @@ -215,7 +215,7 @@ diff --git a/_o_m_sim_i_b_d_8cc.html b/_o_m_sim_i_b_d_8cc.html index b3c4012608..31140c1ec3 100644 --- a/_o_m_sim_i_b_d_8cc.html +++ b/_o_m_sim_i_b_d_8cc.html @@ -129,7 +129,7 @@ diff --git a/_o_m_sim_i_b_d_8hh.html b/_o_m_sim_i_b_d_8hh.html index 3d3c7aa895..31cad110e4 100644 --- a/_o_m_sim_i_b_d_8hh.html +++ b/_o_m_sim_i_b_d_8hh.html @@ -173,7 +173,7 @@

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diff --git a/class_o_m_sim_stepping_action-members.html b/class_o_m_sim_stepping_action-members.html index 1c5ec8f602..671f4c2702 100644 --- a/class_o_m_sim_stepping_action-members.html +++ b/class_o_m_sim_stepping_action-members.html @@ -128,7 +128,7 @@ diff --git a/class_o_m_sim_stepping_action.html b/class_o_m_sim_stepping_action.html index 48af715883..26dc10dd98 100644 --- a/class_o_m_sim_stepping_action.html +++ b/class_o_m_sim_stepping_action.html @@ -229,7 +229,7 @@

  • OMSimSteppingAction
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_o_m_sim_tracking_action-members.html b/class_o_m_sim_tracking_action-members.html index feb44a0d0b..a6c1dc72c5 100644 --- a/class_o_m_sim_tracking_action-members.html +++ b/class_o_m_sim_tracking_action-members.html @@ -129,7 +129,7 @@ diff --git a/class_o_m_sim_tracking_action.html b/class_o_m_sim_tracking_action.html index 7413503659..01d002be79 100644 --- a/class_o_m_sim_tracking_action.html +++ b/class_o_m_sim_tracking_action.html @@ -250,7 +250,7 @@

  • OMSimTrackingAction
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_o_m_sim_u_iinterface-members.html b/class_o_m_sim_u_iinterface-members.html index e6c48ec45c..dc5c6bc435 100644 --- a/class_o_m_sim_u_iinterface-members.html +++ b/class_o_m_sim_u_iinterface-members.html @@ -136,7 +136,7 @@ diff --git a/class_o_m_sim_u_iinterface.html b/class_o_m_sim_u_iinterface.html index 9e66adfebb..36999c8116 100644 --- a/class_o_m_sim_u_iinterface.html +++ b/class_o_m_sim_u_iinterface.html @@ -568,7 +568,7 @@

  • OMSimUIinterface
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_optical_module-members.html b/class_optical_module-members.html index 54fbd23878..faa09abc7f 100644 --- a/class_optical_module-members.html +++ b/class_optical_module-members.html @@ -165,7 +165,7 @@ diff --git a/class_optical_module.html b/class_optical_module.html index c0880dba1b..4fe8ddb4cc 100644 --- a/class_optical_module.html +++ b/class_optical_module.html @@ -388,7 +388,7 @@

  • OpticalModule
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_parameter_table-members.html b/class_parameter_table-members.html index b1eacc7864..92de68a30f 100644 --- a/class_parameter_table-members.html +++ b/class_parameter_table-members.html @@ -134,7 +134,7 @@ diff --git a/class_parameter_table.html b/class_parameter_table.html index bdb0d8bf12..7c8299770e 100644 --- a/class_parameter_table.html +++ b/class_parameter_table.html @@ -490,7 +490,7 @@

  • ParameterTable
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_reflective_surface-members.html b/class_reflective_surface-members.html index 83fd3fde09..307d3ecf17 100644 --- a/class_reflective_surface-members.html +++ b/class_reflective_surface-members.html @@ -138,7 +138,7 @@ diff --git a/class_reflective_surface.html b/class_reflective_surface.html index 1ca2831b33..7acd8af036 100644 --- a/class_reflective_surface.html +++ b/class_reflective_surface.html @@ -335,7 +335,7 @@

  • ReflectiveSurface
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_refraction_and_absorption-members.html b/class_refraction_and_absorption-members.html index 25e001e2ae..196d7cf2aa 100644 --- a/class_refraction_and_absorption-members.html +++ b/class_refraction_and_absorption-members.html @@ -142,7 +142,7 @@ diff --git a/class_refraction_and_absorption.html b/class_refraction_and_absorption.html index 5d818a4aea..4791911262 100644 --- a/class_refraction_and_absorption.html +++ b/class_refraction_and_absorption.html @@ -254,7 +254,7 @@

  • RefractionAndAbsorption
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_refraction_only-members.html b/class_refraction_only-members.html index 38a5efa907..8e30910c67 100644 --- a/class_refraction_only-members.html +++ b/class_refraction_only-members.html @@ -142,7 +142,7 @@ diff --git a/class_refraction_only.html b/class_refraction_only.html index 94b0ed8859..ad23368b9c 100644 --- a/class_refraction_only.html +++ b/class_refraction_only.html @@ -255,7 +255,7 @@

  • RefractionOnly
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/class_scintillation_properties-members.html b/class_scintillation_properties-members.html index e8df5b5e2e..42474a5903 100644 --- a/class_scintillation_properties-members.html +++ b/class_scintillation_properties-members.html @@ -144,7 +144,7 @@ diff --git a/class_scintillation_properties.html b/class_scintillation_properties.html index 819a22d94b..3288de07b6 100644 --- a/class_scintillation_properties.html +++ b/class_scintillation_properties.html @@ -612,7 +612,7 @@

  • ScintillationProperties
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classabc_data_file-members.html b/classabc_data_file-members.html index f4396869e5..8a09774482 100644 --- a/classabc_data_file-members.html +++ b/classabc_data_file-members.html @@ -133,7 +133,7 @@ diff --git a/classabc_data_file.html b/classabc_data_file.html index aaa9641c07..2f91fe5429 100644 --- a/classabc_data_file.html +++ b/classabc_data_file.html @@ -373,7 +373,7 @@

  • abcDataFile
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classabc_detector_component-members.html b/classabc_detector_component-members.html index 8ef9ea2afe..f3bb09c92a 100644 --- a/classabc_detector_component-members.html +++ b/classabc_detector_component-members.html @@ -160,7 +160,7 @@ diff --git a/classabc_detector_component.html b/classabc_detector_component.html index d2cda287a1..32f6fa183d 100644 --- a/classabc_detector_component.html +++ b/classabc_detector_component.html @@ -1174,7 +1174,7 @@

  • abcDetectorComponent
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classabc_material_data-members.html b/classabc_material_data-members.html index 410a67dc6d..0593bb64c8 100644 --- a/classabc_material_data-members.html +++ b/classabc_material_data-members.html @@ -141,7 +141,7 @@ diff --git a/classabc_material_data.html b/classabc_material_data.html index be31f2c192..29fa784a4e 100644 --- a/classabc_material_data.html +++ b/classabc_material_data.html @@ -390,7 +390,7 @@

  • abcMaterialData
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classes.html b/classes.html index 35d550f0dd..bc88776129 100644 --- a/classes.html +++ b/classes.html @@ -176,7 +176,7 @@ diff --git a/classm_d_o_m-members.html b/classm_d_o_m-members.html index ac85076557..54e3c907b9 100644 --- a/classm_d_o_m-members.html +++ b/classm_d_o_m-members.html @@ -211,7 +211,7 @@ diff --git a/classm_d_o_m.html b/classm_d_o_m.html index 4446334182..f6a97f26c3 100644 --- a/classm_d_o_m.html +++ b/classm_d_o_m.html @@ -1487,7 +1487,7 @@

  • mDOM
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classm_d_o_m_flasher-members.html b/classm_d_o_m_flasher-members.html index 957dab9f78..49174dbf22 100644 --- a/classm_d_o_m_flasher-members.html +++ b/classm_d_o_m_flasher-members.html @@ -179,7 +179,7 @@ diff --git a/classm_d_o_m_flasher.html b/classm_d_o_m_flasher.html index c41f3a9de1..9d762022b5 100644 --- a/classm_d_o_m_flasher.html +++ b/classm_d_o_m_flasher.html @@ -806,7 +806,7 @@

  • mDOMFlasher
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classm_d_o_m_harness-members.html b/classm_d_o_m_harness-members.html index 6934cf84f1..f13fde4fe5 100644 --- a/classm_d_o_m_harness-members.html +++ b/classm_d_o_m_harness-members.html @@ -180,7 +180,7 @@ diff --git a/classm_d_o_m_harness.html b/classm_d_o_m_harness.html index 10c0765bc2..5efd9f36b8 100644 --- a/classm_d_o_m_harness.html +++ b/classm_d_o_m_harness.html @@ -788,7 +788,7 @@

  • mDOMHarness
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/classp_d_o_m-members.html b/classp_d_o_m-members.html index 90ec1c5ee8..bcefca25ac 100644 --- a/classp_d_o_m-members.html +++ b/classp_d_o_m-members.html @@ -168,7 +168,7 @@ diff --git a/classp_d_o_m.html b/classp_d_o_m.html index a181627b6b..65edd858dd 100644 --- a/classp_d_o_m.html +++ b/classp_d_o_m.html @@ -419,7 +419,7 @@

  • pDOM
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000002_000003.html b/dir_000002_000003.html index 24ad803bdc..d127937191 100644 --- a/dir_000002_000003.html +++ b/dir_000002_000003.html @@ -119,7 +119,7 @@

src → include Relation

  • common
  • framework
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000004_000000.html b/dir_000004_000000.html index 7d23ad610c..9c609228df 100644 --- a/dir_000004_000000.html +++ b/dir_000004_000000.html @@ -119,7 +119,7 @@

effective_area → common Relation

  • effective_area
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000004_000008.html b/dir_000004_000008.html index c620645e95..034c3da95c 100644 --- a/dir_000004_000008.html +++ b/dir_000004_000008.html @@ -119,7 +119,7 @@

effective_area → include Relation

  • effective_area
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000005_000010.html b/dir_000005_000010.html index 0b2451ee4d..13705a748d 100644 --- a/dir_000005_000010.html +++ b/dir_000005_000010.html @@ -119,7 +119,7 @@

radioactive_decays → include Relation

  • radioactive_decays
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000007_000000.html b/dir_000007_000000.html index 7a9b88ab94..ae9c4d81ee 100644 --- a/dir_000007_000000.html +++ b/dir_000007_000000.html @@ -119,7 +119,7 @@

src → common Relation

  • effective_area
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000007_000008.html b/dir_000007_000008.html index b16d74f53a..b45729cb64 100644 --- a/dir_000007_000008.html +++ b/dir_000007_000008.html @@ -119,7 +119,7 @@

src → include Relation

  • effective_area
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000008_000000.html b/dir_000008_000000.html index c1d12eb7f3..7affa25e19 100644 --- a/dir_000008_000000.html +++ b/dir_000008_000000.html @@ -119,7 +119,7 @@

include → common Relation

diff --git a/dir_000009_000000.html b/dir_000009_000000.html index 2ccf2d25b5..e1603f5b19 100644 --- a/dir_000009_000000.html +++ b/dir_000009_000000.html @@ -119,7 +119,7 @@

src → common Relation

  • radioactive_decays
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000009_000010.html b/dir_000009_000010.html index 2ca175acfd..0a667aec46 100644 --- a/dir_000009_000010.html +++ b/dir_000009_000010.html @@ -119,7 +119,7 @@

src → include Relation

  • radioactive_decays
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000010_000000.html b/dir_000010_000000.html index fbeba05fe9..18c67ef9ea 100644 --- a/dir_000010_000000.html +++ b/dir_000010_000000.html @@ -119,7 +119,7 @@

include → common Relation

diff --git a/dir_000011_000001.html b/dir_000011_000001.html index 242429fa37..9901aa4d3e 100644 --- a/dir_000011_000001.html +++ b/dir_000011_000001.html @@ -119,7 +119,7 @@

optical_modules → framework Relation

  • common
  • optical_modules
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000012_000001.html b/dir_000012_000001.html index e20d603fb2..e60a3cc5bd 100644 --- a/dir_000012_000001.html +++ b/dir_000012_000001.html @@ -119,7 +119,7 @@

src → framework Relation

< diff --git a/dir_000012_000013.html b/dir_000012_000013.html index fed21ecc84..eca4a5b385 100644 --- a/dir_000012_000013.html +++ b/dir_000012_000013.html @@ -119,7 +119,7 @@

src → include Relation

  • common
  • optical_modules
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000013_000001.html b/dir_000013_000001.html index 729f1c03eb..39152eb4b0 100644 --- a/dir_000013_000001.html +++ b/dir_000013_000001.html @@ -119,7 +119,7 @@

include → framework Relation

  • common
  • optical_modules
  • include
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000014_000000.html b/dir_000014_000000.html index 218242119a..0c1f29f9fa 100644 --- a/dir_000014_000000.html +++ b/dir_000014_000000.html @@ -119,7 +119,7 @@

src → common Relation

  • supernova
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000014_000015.html b/dir_000014_000015.html index 257a3c1537..7dee06c2c4 100644 --- a/dir_000014_000015.html +++ b/dir_000014_000015.html @@ -119,7 +119,7 @@

src → include Relation

  • supernova
  • src
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/dir_000015_000000.html b/dir_000015_000000.html index a6223581b8..46a377f10b 100644 --- a/dir_000015_000000.html +++ b/dir_000015_000000.html @@ -119,7 +119,7 @@

include → common Relation

diff --git a/dir_0508a806709bbb036eb481438c5edd07.html b/dir_0508a806709bbb036eb481438c5edd07.html index e1b838294b..886377ed17 100644 --- a/dir_0508a806709bbb036eb481438c5edd07.html +++ b/dir_0508a806709bbb036eb481438c5edd07.html @@ -143,7 +143,7 @@ diff --git a/dir_067620130b80b08c0f6387663e9785ff.html b/dir_067620130b80b08c0f6387663e9785ff.html index b3879c7198..c8935ec472 100644 --- a/dir_067620130b80b08c0f6387663e9785ff.html +++ b/dir_067620130b80b08c0f6387663e9785ff.html @@ -146,7 +146,7 @@ diff --git a/dir_1bc21981797ed08ef994409d474646cd.html b/dir_1bc21981797ed08ef994409d474646cd.html index 6b9388d167..cf994b286d 100644 --- a/dir_1bc21981797ed08ef994409d474646cd.html +++ b/dir_1bc21981797ed08ef994409d474646cd.html @@ -165,7 +165,7 @@ diff --git a/dir_3eb80fb40bb9918af86e7507fbd94fb7.html b/dir_3eb80fb40bb9918af86e7507fbd94fb7.html index 89f3e22393..af11305b37 100644 --- a/dir_3eb80fb40bb9918af86e7507fbd94fb7.html +++ b/dir_3eb80fb40bb9918af86e7507fbd94fb7.html @@ -154,7 +154,7 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                                                                                                  - h -

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                                                                                                    - i -

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                                                                                                          - n -

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                                                                                                                          diff --git a/functions_vars_v.html b/functions_vars_v.html index d2d6e910e6..d86ef5384f 100644 --- a/functions_vars_v.html +++ b/functions_vars_v.html @@ -146,7 +146,7 @@

                                                                                                                          - v -

                                                                                                                            diff --git a/functions_vars_w.html b/functions_vars_w.html index 981abdb35c..a8ff8e04f1 100644 --- a/functions_vars_w.html +++ b/functions_vars_w.html @@ -131,7 +131,7 @@

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                                                                                                                                        diff --git a/functions_y.html b/functions_y.html index 6736a4d22a..f89577c0f3 100644 --- a/functions_y.html +++ b/functions_y.html @@ -131,7 +131,7 @@

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                                                                                                                                            - ~ -

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                                                                                                                                                  In the IBD case, the outgoing neutron is not simulated; hence, the neutron capture process that might be detected is not included in the simulation. Each event is assigned a weight based on the interaction probability, detailed later on this page. By default, the surrounding ice is represented as a cylinder facing the CCSN, simplifying the weight calculations.

                                                                                                                                                  Although CCSN models incorporate neutrino oscillations, the default simulation does not include any oscillation scenario in the weight calculations.

                                                                                                                                                    -

                                                                                                                                                  • - Figure 1: Diagram of the steps involved to generate the events for the simulation of CCSN neutrinos. The scheme is valid for both IBD and ENES, except for the threshold check. Here, stands for both electron from ENES or positron from IBD, and ν (este simbolo se vera bien?) for both electronic neutrino from ENES or electronic antineutrino from IBD.. Image from this thesis.

                                                                                                                                                    The detailed procedure for this simulation is comprehensively described in this thesis, specifically in section 6.4. Below is a summary extracted from this source, outlining the steps taken to generate the events:

                                                                                                                                                    -

                                                                                                                                                    \begin{enumerate} \item Utilizing the models, the expected flux per area is calculated from the luminosity (L(t)) and the mean energy (\bar{E}(t)) according to \begin{equation} \label{eq:fluxes} \Phi (t) = \frac{1}{4\pi d^2} \cdot \frac{L(t)}{\bar{E}(t)}. \end{equation}

                                                                                                                                                    -

                                                                                                                                                    \item The distribution of (\Phi (t)) is used to sample a time (t) of the burst via the inverse CDF (Cumulative Distribution Function) method. All other sampling from distributions within this simulation also employs the inverse CDF method.

                                                                                                                                                    -

                                                                                                                                                    \item For the sampled time (t), the corresponding mean energy and mean squared energy are extracted from the models. These parameters contribute to the construction of the energy spectrum (f(E,t)), as elucidated in this paper.

                                                                                                                                                    -

                                                                                                                                                    \item The energy of the neutrino/antineutrino (E_\nu) is sampled from (f(E,t)). If the energy falls below the IBD threshold, the algorithm reverts to the second step.

                                                                                                                                                    -

                                                                                                                                                    \item From (E_\nu), the angular cross section is devised. This informs the sampling of the angle (\theta) between the incoming neutrino and the resulting (e^-/e^+). The (\phi) direction is randomly generated within the range of (0) to (2\pi).

                                                                                                                                                    -

                                                                                                                                                    \item The energy of (e^-/e^+) is deduced from (\theta) and (E_\nu). The interaction probability for such an event is ascertained using the total cross section, facilitating the computation of the interaction weight, as further described below.

                                                                                                                                                    -

                                                                                                                                                    \item The (e^-/e^+) is manifested at a random position within the ice volume. \end{enumerate}

                                                                                                                                                    -
                                                                                                                                                    • +

                                                                                                                                                  • + Figure 1: Diagram of the steps involved to generate the events for the simulation of CCSN neutrinos. The scheme is valid for both IBD and ENES, except for the threshold check. Here, stands for both electron from ENES or positron from IBD, and ν (este simbolo se vera bien?) for both electronic neutrino from ENES or electronic antineutrino from IBD.. Image from this thesis.

                                                                                                                                                    The detailed procedure for this simulation is comprehensively described in this thesis, specifically in section 6.4. Below is a summary extracted from this source, outlining the steps taken to generate the events: 

                                                                                                                                                    1. Utilizing the models, the expected flux per area is calculated from the luminosity 
+\f$L(t)\f$ and the mean energy \f$\bar{E}(t)\f$ according to
+\begin{equation}
+    \label{eq:fluxes}
+    \Phi (t) = \frac{1}{4\pi d^2} \cdot \frac{L(t)}{\bar{E}(t)}.
+\end{equation}
+
+2. The distribution of \f$\Phi (t)\f$ is used to sample a time \f$t\f$ of the burst via 
+the inverse CDF (Cumulative Distribution Function) method. All other sampling from distributions within this simulation 
+also employs the inverse CDF method.
+
+3. For the sampled time \f$t\f$, the corresponding mean energy and mean squared energy 
+are extracted from the models. These parameters contribute to the construction of the 
+energy spectrum \f$f(E,t)\f$, as elucidated in 
+<a href="https://arxiv.org/pdf/1211.3920.pdf">this paper</a>.
+
+4. The energy of the neutrino/antineutrino \f$E_\nu\f$ is sampled from \f$f(E,t)\f$. 
+If the energy falls below the IBD threshold, the algorithm reverts to the second step.
+
+5. From \f$E_\nu\f$, the angular cross section is devised. This informs the sampling 
+of the angle \f$\theta\f$ between the incoming neutrino and the resulting \f$e^-/e^+\f$. 
+The \‍(\phi\‍) direction is randomly generated within the range of \f$0\f$ to \f$2\pi\f$.
+
+6. The energy of \f$e^-/e^+\f$ is deduced from \f$\theta\f$ and \f$E_\nu\f$. The interaction 
+probability for such an event is ascertained using the total cross section, 
+facilitating the computation of the interaction weight, as further described below.
+
+7. The \f$e^-/e^+\f$ is manifested at a random position within the ice volume.
+

                                                                                                                                                  Parameters

                                                                                                                                                  @@ -149,28 +169,35 @@

                                                                                                                                                  "./OMSim_supernova -n 100 --wheight 20 --wradius 20 --depth_pos 75 -o outputfilename --SNgun 0 --SNtype 0"

                                                                                                                                                  Parameters

                                                                                                                                                  -

                                                                                                                                                  \begin{itemize} \item -n: Number of particles to be generated. \item –depth_pos: Index of the vector determining the depth of the simulated modules. Notable values include DustLayer=65, MeanICUProperties(approx)=75, and CleanestIce=88. The data is located in "common/data/Materials/IceCubeICE.dat". The "jDepth_spice" vector provides the depth, with depth_pos serving as the index. This selection affects the effective scattering and absorption lengths of the ice at the specified depth. \item -o: Output file name. By default, two output files are created: one containing the simulated event information, and another with detection data. \end{itemize}

                                                                                                                                                  +

                                                                                                                                                  -n: Number of particles to be generated. –depth_pos: Index of the vector determining the depth of the simulated modules. Notable values include DustLayer=65, MeanICUProperties(approx)=75, and CleanestIce=88. The data is located in "common/data/Materials/IceCubeICE.dat". The "jDepth_spice" vector provides the depth, with depth_pos serving as the index. This selection affects the effective scattering and absorption lengths of the ice at the specified depth. -o: Output file name. By default, two output files are created: one containing the simulated event information, and another with detection data.

                                                                                                                                                  Framework Parameters

                                                                                                                                                  -

                                                                                                                                                  \begin{itemize} \item –wheight: Height of the ice's simulated world cylinder. \item –wradius: Radius of the ice's simulated world cylinder. \item –SNgun: Chooses the interaction type (0 for IBD, 1 for ENES). \item –SNtype: Selects the CCSN model. Two models are currently available, provided by the Garching group. These models represent the expected fluxes from two CCSNs resulting in neutron stars, with different progenitor masses (27 and 9.6 solar masses). Simulations yielding this data can be found at https://arxiv.org/abs/1510.04643 \end{itemize}

                                                                                                                                                  +

                                                                                                                                                  –wheight: Height of the ice's simulated world cylinder. –wradius: Radius of the ice's simulated world cylinder. –SNgun: Chooses the interaction type (0 for IBD, 1 for ENES). –SNtype: Selects the CCSN model. Two models are currently available, provided by the Garching group. These models represent the expected fluxes from two CCSNs resulting in neutron stars, with different progenitor masses (27 and 9.6 solar masses). Simulations yielding this data can be found at https://arxiv.org/abs/1510.04643

                                                                                                                                                  Energy Studies

                                                                                                                                                  This section allows users to manually set the mean energy of generated events by providing specific input parameters. For instance:

                                                                                                                                                  "--SNfixEnergy --SNmeanE 10.0 --SNalpha 3.0"

                                                                                                                                                  -

                                                                                                                                                  \begin{itemize} \item –SNfixEnergy: Acts as a flag parameter. When invoked, the simulation disregards the actual mean energy of neutrinos corresponding to the burst time. Instead, it adopts the mean energy and the pinching parameter specified by the subsequent two parameters. \item –SNmeanE: Specifies the mean energy of the neutrinos. \item –SNalpha: Defines the pinching parameter of the energy distribution (see this paper). \end{itemize}

                                                                                                                                                  +

                                                                                                                                                  –SNfixEnergy: Acts as a flag parameter. When invoked, the simulation disregards the actual mean energy of neutrinos corresponding to the burst time. Instead, it adopts the mean energy and the pinching parameter specified by the subsequent two parameters. –SNmeanE: Specifies the mean energy of the neutrinos. –SNalpha: Defines the pinching parameter of the energy distribution (see this paper).

                                                                                                                                                  Consequently, the neutrinos' energy is sampled from the distribution, derived from these two parameters and the previously mentioned model.

                                                                                                                                                  Files

                                                                                                                                                  Information regarding the files that contain data outputs and insights derived from the simulated neutrino events.

                                                                                                                                                  -

                                                                                                                                                  This file encapsulates data concerning each generated neutrino event. Each entry contains:

                                                                                                                                                  -

                                                                                                                                                  \begin{itemize} \item Time of the neutrino burst. \item Corresponding mean energy derived from the model. \item Sampled neutrino energy (E_\nu). \item (\cos(\theta)), where (\theta) is the angle between the incoming neutrino and the outgoing particle (e- or e+). \item Energy of the outgoing particle (e- or e+). \item Interaction weight, calculated using the formula: [ W_{\mathrm{int}}(E_\nu) = \sigma(E) \cdot n_{\mathrm{target}} \cdot l, ] where:

                                                                                                                                                    -
                                                                                                                                                  • (\sigma(E)) is the total cross section for the interaction,
                                                                                                                                                    • -
                                                                                                                                                  • (n_{\mathrm{target}}) is the number of targets available for the interaction in the ice,
                                                                                                                                                    • -
                                                                                                                                                  • (l) is the length of the simulated cylindrical world. \end{itemize}
                                                                                                                                                    • -
                                                                                                                                                  -

                                                                                                                                                  +

                                                                                                                                                  This file encapsulates data concerning each generated neutrino event. Each entry contains: 

                                                                                                                                                  - Time of the neutrino burst.
+- Corresponding mean energy derived from the model.
+- Sampled neutrino energy \f$E_\nu\f$.
+- \f$\cos(\theta)\f$, where \f$\theta\f$ is the angle between the incoming neutrino and the outgoing particle (e- or e+).
+- Energy of the outgoing particle (e- or e+).
+- Interaction weight, calculated using the formula:
+    \[
+    W_{\mathrm{int}}(E_\nu) = \sigma(E) \cdot n_{\mathrm{target}} \cdot l,
+    \]
+    where:
+    - \‍(\sigma(E)\‍) is the total cross section for the interaction,
+    - \‍(n_{\mathrm{target}}\‍) is the number of targets available for the interaction in the ice,
+    - \‍(l\‍) is the length of the simulated cylindrical world.
+

                                                                                                                                                  This file contains the detection information. Its structure is designed to facilitate various trigger studies, allowing the examination of different time windows. Users might evaluate its structure for convenience, particularly if the trigger check is integrated within the simulation (requiring a predefined time window).

                                                                                                                                                  The default content structure is as follows: [ \text{Total hits | Modules hit | PMTs hit | ...for each PMT hit...| Module number | PMT number | Hits in that PMT | "...for each Hit..." << " hit time |"} ]

                                                                                                                                                  @@ -181,13 +208,42 @@

                                                                                                                                                  These weight factors can be added similarly as explained in this thesis, section 6.4.2.

                                                                                                                                                  The total weight is composed of 3 components: the interaction probability, the SN flux through the simulated volume, and the different optical properties of the modules at different depths:

                                                                                                                                                  \begin{equation} \label{eq:sn_weights} W = W_{\mathrm{int}}(E) \cdot W_{\mathrm{flux}}(d) \cdot W_{\mathrm{eff}}. \end{equation}

                                                                                                                                                  -

                                                                                                                                                  Each component is explained as follows:

                                                                                                                                                  -

                                                                                                                                                  \begin{itemize} \item Interaction Probability Weight: \begin{equation} \label{eq:sn_weight_int} W_{\mathrm{int}}(E_\nu) = \sigma(E) \cdot n_{\mathrm{target}} \cdot l, \end{equation} where (\sigma(E_\nu)) is the total cross section for the interaction, (n_{\mathrm{target}}) is the number of targets per unit of volume for such interaction, and (l=40\,m) is the length of the generation volume along the neutrino direction axis. This is the length of the cylinder facing the CCSN.

                                                                                                                                                  -

                                                                                                                                                  \item Flux Weight: \begin{equation} \label{eq:sn_weight_flux} W_{\mathrm{flux}} = \frac{1}{N_{\mathrm{gen}}} \cdot \frac{r^2}{d^2} \cdot \int \frac{L(t)}{\bar{E}(t)} dt, \end{equation} where (r=20\,m) is the cylindrical generation volume’s radius, (d) is the distance from Earth where the CCSN is assumed to occur, and (N_{\mathrm{gen}}) is the number of generated events.

                                                                                                                                                  -

                                                                                                                                                  \item Effective Weight: \begin{equation} \label{eq:sn_weight_eff} W_{\mathrm{eff}} = N_{\mathrm{modules}} \cdot \frac{\bar{V}_{\mathrm{eff}}(m)}{V_{\mathrm{eff}}(m,z_{\mathrm{sim}})}, \end{equation} where (N_{\mathrm{modules}}) is the total modules in the simulated detector, (V_{\mathrm{eff}}(m, z_{\mathrm{sim}})) is the effective volume at the simulation depth, and (\bar{V}_{\mathrm{eff}}(m)) is the mean effective volume for all modules in the detector. The term (m) represents multiplicity, defined as the count of different PMTs within a single module that detected the event within a specific time window. \end{itemize}

                                                                                                                                                  -

                                                                                                                                                  The effective volume can be calculated in different ways. Old simulations of the mDOM, described in this thesis, section 6.3, were used in past studies. A linear regression of the effective volume concerning the absorption length, derived from various depths, provides each depth's effective volume. Although it is advisable to redo these simulations with a current mDOM model, users can temporarily use the old data with a regression line of (V_{\mathrm{eff}} = b \cdot x + c), where (x = 1/a) is the inverse of the absorption length. The coefficients (b) and (c), depending on the event's multiplicity, were obtained as follows:

                                                                                                                                                  -

                                                                                                                                                  \begin{center} \begin{tabular}{|c|c|c|} \hline PMTs & b (slope, units (m^2)) & c (units (m^3)) \ \hline 1 & 15.184 & 0.000 \ 2 & 0.135 & 47.005 \ 3 & 0.031 & 16.170 \ 4 & 0.010 & 8.680 \ 5 & 0.004 & 5.105 \ (\geq6) & 0.003 & 2.909 \ \hline \end{tabular} \end{center}

                                                                                                                                                  -

                                                                                                                                                  Note that, for more than 5 PMTs, the same fit line is employed due to insufficient statistics at higher PMTs in the effective volume simulation. Additionally, since the absorption length depends on the wavelength, the fits above were obtained assuming a wavelength of (\lambda = 400\,nm).

                                                                                                                                                  +

                                                                                                                                                  Each component is explained as follows: 

                                                                                                                                                  - Interaction Probability Weight:
+    \begin{equation}
+        \label{eq:sn_weight_int}
+        W_{\mathrm{int}}(E_\nu) = \sigma(E) \cdot n_{\mathrm{target}} \cdot l,
+    \end{equation}
+    where \‍(\sigma(E_\nu)\‍) is the total cross section for the interaction, \‍(n_{\mathrm{target}}\‍) is the 
+    number of targets per unit of volume for such interaction, and \‍(l=40\,m\‍) is the length of the generation 
+    volume along the neutrino direction axis. This is the length of the cylinder facing the CCSN.
+
+- Flux Weight:
+    \begin{equation}
+        \label{eq:sn_weight_flux}
+        W_{\mathrm{flux}} =  \frac{1}{N_{\mathrm{gen}}} \cdot \frac{r^2}{d^2} \cdot \int \frac{L(t)}{\bar{E}(t)} dt,
+    \end{equation}
+    where \‍(r=20\,m\‍) is the cylindrical generation volume’s radius, \‍(d\‍) is the distance from Earth where the 
+    CCSN is assumed to occur, and \‍(N_{\mathrm{gen}}\‍) is the number of generated events.
+
+- Effective Weight:
+    \begin{equation}
+        \label{eq:sn_weight_eff}
+        W_{\mathrm{eff}} = N_{\mathrm{modules}} \cdot \frac{\bar{V}_{\mathrm{eff}}(m)}{V_{\mathrm{eff}}(m,z_{\mathrm{sim}})},
+    \end{equation}
+    where \‍(N_{\mathrm{modules}}\‍) is the total modules in the simulated detector, \‍(V_{\mathrm{eff}}(m, 
+    z_{\mathrm{sim}})\‍) is the effective volume at the simulation depth, and \‍(\bar{V}_{\mathrm{eff}}(m)\‍) is 
+    the mean effective volume for all modules in the detector. The term \‍(m\‍) represents multiplicity, defined 
+    as the count of different PMTs within a single module that detected the event within a specific time window.
+

                                                                                                                                                  The effective volume can be calculated in different ways. Old simulations of the mDOM, described in this thesis, section 6.3, were used in past studies. A linear regression of the effective volume concerning the absorption length, derived from various depths, provides each depth's effective volume. Although it is advisable to redo these simulations with a current mDOM model, users can temporarily use the old data with a regression line of \(V_{\mathrm{eff}} = b \cdot x + c\), where \(x = 1/a\) is the inverse of the absorption length. The coefficients \(b\) and \(c\), depending on the event's multiplicity, were obtained as follows:

                                                                                                                                                  +
                                                                                                                                                  *  | multiplicity |     b (slope, m^2)         |      c (m^3)     |
+*  |--------------|----------------------------|------------------|
+*  |      1       |          15.1843           |   0.000 (imposed)|
+*  |      2       |           0.1352           |      47.005      |
+*  |      3       |           0.0306           |      16.170      |
+*  |      4       |           0.0095           |       8.680      |
+*  |      5       |           0.0039           |       5.105      |
+*  |     >= 6     |           0.0026           |       2.909      |
+*

                                                                                                                                                  Note that, for more than 5 PMTs, the same fit line is employed due to insufficient statistics at higher PMTs in the effective volume simulation. Additionally, since the absorption length depends on the wavelength, the fits above were obtained assuming a wavelength of \(\lambda = 400\,nm\).

@@ -200,7 +256,7 @@

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The scheme is valid for both IBD and ENES, except for the threshold check. Here, stands for both electron from ENES or positron from IBD, and ν (este simbolo se vera bien?) for both electronic neutrino from ENES or electronic antineutrino from IBD.. Image from \href{https://zenodo.org/record/8107177}{\texttt{ this thesis}}.} -The detailed procedure for this simulation is comprehensively described in \href{https://zenodo.org/record/8107177}{\texttt{ this thesis}}, specifically in section 6.\+4. Below is a summary extracted from this source, outlining the steps taken to generate the events\+: +The detailed procedure for this simulation is comprehensively described in \href{https://zenodo.org/record/8107177}{\texttt{ this thesis}}, specifically in section 6.\+4. Below is a summary extracted from this source, outlining the steps taken to generate the events\+: \begin{DoxyVerb}1. Utilizing the models, the expected flux per area is calculated from the luminosity +\f$L(t)\f$ and the mean energy \f$\bar{E}(t)\f$ according to +\begin{equation} + \label{eq:fluxes} + \Phi (t) = \frac{1}{4\pi d^2} \cdot \frac{L(t)}{\bar{E}(t)}. +\end{equation} -\textbackslash{}begin\{enumerate\} \textbackslash{}item Utilizing the models, the expected flux per area is calculated from the luminosity (L(t)) and the mean energy (\textbackslash{}bar\{E\}(t)) according to \textbackslash{}begin\{equation\} \textbackslash{}label\{eq\+:fluxes\} \textbackslash{}\+Phi (t) = \textbackslash{}frac\{1\}\{4\textbackslash{}pi d$^\wedge$2\} \textbackslash{}cdot \textbackslash{}frac\{L(t)\}\{\textbackslash{}bar\{E\}(t)\}. \textbackslash{}end\{equation\} +2. The distribution of \f$\Phi (t)\f$ is used to sample a time \f$t\f$ of the burst via +the inverse CDF (Cumulative Distribution Function) method. All other sampling from distributions within this simulation +also employs the inverse CDF method. -\textbackslash{}item The distribution of (\textbackslash{}\+Phi (t)) is used to sample a time (t) of the burst via the inverse CDF (Cumulative Distribution Function) method. All other sampling from distributions within this simulation also employs the inverse CDF method. +3. For the sampled time \f$t\f$, the corresponding mean energy and mean squared energy +are extracted from the models. These parameters contribute to the construction of the +energy spectrum \f$f(E,t)\f$, as elucidated in +this paper. -\textbackslash{}item For the sampled time (t), the corresponding mean energy and mean squared energy are extracted from the models. These parameters contribute to the construction of the energy spectrum (f(\+E,t)), as elucidated in \href{https://arxiv.org/pdf/1211.3920.pdf}{\texttt{ this paper}}. +4. The energy of the neutrino/antineutrino \f$E_\nu\f$ is sampled from \f$f(E,t)\f$. +If the energy falls below the IBD threshold, the algorithm reverts to the second step. -\textbackslash{}item The energy of the neutrino/antineutrino (E\+\_\+\textbackslash{}nu) is sampled from (f(\+E,t)). If the energy falls below the IBD threshold, the algorithm reverts to the second step. +5. From \f$E_\nu\f$, the angular cross section is devised. This informs the sampling +of the angle \f$\theta\f$ between the incoming neutrino and the resulting \f$e^-/e^+\f$. +The \(\phi\) direction is randomly generated within the range of \f$0\f$ to \f$2\pi\f$. -\textbackslash{}item From (E\+\_\+\textbackslash{}nu), the angular cross section is devised. This informs the sampling of the angle (\textbackslash{}theta) between the incoming neutrino and the resulting (e$^\wedge$-\//e$^\wedge$+). The (\textbackslash{}phi) direction is randomly generated within the range of (0) to (2\textbackslash{}pi). +6. The energy of \f$e^-/e^+\f$ is deduced from \f$\theta\f$ and \f$E_\nu\f$. The interaction +probability for such an event is ascertained using the total cross section, +facilitating the computation of the interaction weight, as further described below. -\textbackslash{}item The energy of (e$^\wedge$-\//e$^\wedge$+) is deduced from (\textbackslash{}theta) and (E\+\_\+\textbackslash{}nu). The interaction probability for such an event is ascertained using the total cross section, facilitating the computation of the interaction weight, as further described below. +7. The \f$e^-/e^+\f$ is manifested at a random position within the ice volume. +\end{DoxyVerb} -\textbackslash{}item The (e$^\wedge$-\//e$^\wedge$+) is manifested at a random position within the ice volume. \textbackslash{}end\{enumerate\} \end{DoxyItemize}\hypertarget{group__sngroup_Input}{}\doxysubsection{Parameters}\label{group__sngroup_Input} Execute {\ttfamily ./\+OMSim\+\_\+supernova -\/-\/help} to display all possible input parameters. A typical command to run the simulation is\+: \char`\"{}./\+OMSim\+\_\+supernova -\/n 100 -\/-\/wheight 20 -\/-\/wradius 20 -\/-\/depth\+\_\+pos 75 -\/o outputfilename -\/-\/\+SNgun 0 -\/-\/\+SNtype 0\char`\"{}\hypertarget{group__sngroup_General}{}\doxysubsubsection{Parameters}\label{group__sngroup_General} -\textbackslash{}begin\{itemize\} \textbackslash{}item -\/n\+: Number of particles to be generated. \textbackslash{}item --depth\+\_\+pos\+: Index of the vector determining the depth of the simulated modules. Notable values include Dust\+Layer=65, Mean\+ICUProperties(approx)=75, and Cleanest\+Ice=88. The data is located in \char`\"{}common/data/\+Materials/\+Ice\+Cube\+ICE.\+dat\char`\"{}. The \char`\"{}j\+Depth\+\_\+spice\char`\"{} vector provides the depth, with depth\+\_\+pos serving as the index. This selection affects the effective scattering and absorption lengths of the ice at the specified depth. \textbackslash{}item -\/o\+: Output file name. By default, two output files are created\+: one containing the simulated event information, and another with detection data. \textbackslash{}end\{itemize\}\hypertarget{group__sngroup_SN}{}\doxysubsubsection{Framework Parameters}\label{group__sngroup_SN} -\textbackslash{}begin\{itemize\} \textbackslash{}item --wheight\+: Height of the ice\textquotesingle{}s simulated world cylinder. \textbackslash{}item --wradius\+: Radius of the ice\textquotesingle{}s simulated world cylinder. \textbackslash{}item --SNgun\+: Chooses the interaction type (0 for IBD, 1 for ENES). \textbackslash{}item --SNtype\+: Selects the CCSN model. Two models are currently available, provided by the Garching group. These models represent the expected fluxes from two CCSNs resulting in neutron stars, with different progenitor masses (27 and 9.\+6 solar masses). Simulations yielding this data can be found at \href{https://arxiv.org/abs/1510.04643}{\texttt{ https\+://arxiv.\+org/abs/1510.\+04643}} \textbackslash{}end\{itemize\}\hypertarget{group__sngroup_Fixed}{}\doxysubsubsection{Energy Studies}\label{group__sngroup_Fixed} +-\/n\+: Number of particles to be generated. --depth\+\_\+pos\+: Index of the vector determining the depth of the simulated modules. Notable values include Dust\+Layer=65, Mean\+ICUProperties(approx)=75, and Cleanest\+Ice=88. The data is located in \char`\"{}common/data/\+Materials/\+Ice\+Cube\+ICE.\+dat\char`\"{}. The \char`\"{}j\+Depth\+\_\+spice\char`\"{} vector provides the depth, with depth\+\_\+pos serving as the index. This selection affects the effective scattering and absorption lengths of the ice at the specified depth. -\/o\+: Output file name. By default, two output files are created\+: one containing the simulated event information, and another with detection data.\hypertarget{group__sngroup_SN}{}\doxysubsubsection{Framework Parameters}\label{group__sngroup_SN} +--wheight\+: Height of the ice\textquotesingle{}s simulated world cylinder. --wradius\+: Radius of the ice\textquotesingle{}s simulated world cylinder. --SNgun\+: Chooses the interaction type (0 for IBD, 1 for ENES). --SNtype\+: Selects the CCSN model. Two models are currently available, provided by the Garching group. These models represent the expected fluxes from two CCSNs resulting in neutron stars, with different progenitor masses (27 and 9.\+6 solar masses). Simulations yielding this data can be found at \href{https://arxiv.org/abs/1510.04643}{\texttt{ https\+://arxiv.\+org/abs/1510.\+04643}}\hypertarget{group__sngroup_Fixed}{}\doxysubsubsection{Energy Studies}\label{group__sngroup_Fixed} This section allows users to manually set the mean energy of generated events by providing specific input parameters. For instance\+: \char`\"{}-\/-\/\+SNfix\+Energy -\/-\/\+SNmean\+E 10.\+0 -\/-\/\+SNalpha 3.\+0\char`\"{} -\textbackslash{}begin\{itemize\} \textbackslash{}item --SNfix\+Energy\+: Acts as a flag parameter. When invoked, the simulation disregards the actual mean energy of neutrinos corresponding to the burst time. Instead, it adopts the mean energy and the pinching parameter specified by the subsequent two parameters. \textbackslash{}item --SNmeanE\+: Specifies the mean energy of the neutrinos. \textbackslash{}item --SNalpha\+: Defines the pinching parameter of the energy distribution (see \href{https://arxiv.org/pdf/1211.3920.pdf}{\texttt{ this paper}}). \textbackslash{}end\{itemize\} +--SNfix\+Energy\+: Acts as a flag parameter. When invoked, the simulation disregards the actual mean energy of neutrinos corresponding to the burst time. Instead, it adopts the mean energy and the pinching parameter specified by the subsequent two parameters. --SNmeanE\+: Specifies the mean energy of the neutrinos. --SNalpha\+: Defines the pinching parameter of the energy distribution (see \href{https://arxiv.org/pdf/1211.3920.pdf}{\texttt{ this paper}}). Consequently, the neutrinos\textquotesingle{} energy is sampled from the distribution, derived from these two parameters and the previously mentioned model.\hypertarget{group__sngroup_Output}{}\doxysubsection{Files}\label{group__sngroup_Output} Information regarding the files that contain data outputs and insights derived from the simulated neutrino events.\hypertarget{_}{}\doxysubsubsection{}\label{_} -This file encapsulates data concerning each generated neutrino event. Each entry contains\+: - -\textbackslash{}begin\{itemize\} \textbackslash{}item Time of the neutrino burst. \textbackslash{}item Corresponding mean energy derived from the model. \textbackslash{}item Sampled neutrino energy (E\+\_\+\textbackslash{}nu). \textbackslash{}item (\textbackslash{}cos(\textbackslash{}theta)), where (\textbackslash{}theta) is the angle between the incoming neutrino and the outgoing particle (e-\/ or e+). \textbackslash{}item Energy of the outgoing particle (e-\/ or e+). \textbackslash{}item Interaction weight, calculated using the formula\+: \mbox{[} W\+\_\+\{\textbackslash{}mathrm\{int\}\}(E\+\_\+\textbackslash{}nu) = \textbackslash{}sigma(E) \textbackslash{}cdot n\+\_\+\{\textbackslash{}mathrm\{target\}\} \textbackslash{}cdot l, \mbox{]} where\+: -\begin{DoxyItemize} -\item (\textbackslash{}sigma(E)) is the total cross section for the interaction, -\item (n\+\_\+\{\textbackslash{}mathrm\{target\}\}) is the number of targets available for the interaction in the ice, -\item (l) is the length of the simulated cylindrical world. \textbackslash{}end\{itemize\} -\end{DoxyItemize}\hypertarget{_}{}\doxyparagraph{}\label{_} +This file encapsulates data concerning each generated neutrino event. Each entry contains\+: \begin{DoxyVerb}- Time of the neutrino burst. +- Corresponding mean energy derived from the model. +- Sampled neutrino energy \f$E_\nu\f$. +- \f$\cos(\theta)\f$, where \f$\theta\f$ is the angle between the incoming neutrino and the outgoing particle (e- or e+). +- Energy of the outgoing particle (e- or e+). +- Interaction weight, calculated using the formula: + \[ + W_{\mathrm{int}}(E_\nu) = \sigma(E) \cdot n_{\mathrm{target}} \cdot l, + \] + where: + - \(\sigma(E)\) is the total cross section for the interaction, + - \(n_{\mathrm{target}}\) is the number of targets available for the interaction in the ice, + - \(l\) is the length of the simulated cylindrical world. +\end{DoxyVerb} + \hypertarget{_}{}\doxyparagraph{}\label{_} This file contains the detection information. Its structure is designed to facilitate various trigger studies, allowing the examination of different time windows. Users might evaluate its structure for convenience, particularly if the trigger check is integrated within the simulation (requiring a predefined time window). The default content structure is as follows\+: \mbox{[} \textbackslash{}text\{Total hits $\vert$ Modules hit $\vert$ PMTs hit $\vert$ ...for each PMT hit...$\vert$ Module number $\vert$ PMT number $\vert$ Hits in that PMT $\vert$ \char`\"{}...\+for each Hit...\char`\"{} $<$$<$ \char`\"{} hit time $\vert$\char`\"{}\} \mbox{]} @@ -77,19 +99,47 @@ \textbackslash{}begin\{equation\} \textbackslash{}label\{eq\+:sn\+\_\+weights\} W = W\+\_\+\{\textbackslash{}mathrm\{int\}\}(E) \textbackslash{}cdot W\+\_\+\{\textbackslash{}mathrm\{flux\}\}(d) \textbackslash{}cdot W\+\_\+\{\textbackslash{}mathrm\{eff\}\}. \textbackslash{}end\{equation\} -Each component is explained as follows\+: - -\textbackslash{}begin\{itemize\} \textbackslash{}item Interaction Probability Weight\+: \textbackslash{}begin\{equation\} \textbackslash{}label\{eq\+:sn\+\_\+weight\+\_\+int\} W\+\_\+\{\textbackslash{}mathrm\{int\}\}(E\+\_\+\textbackslash{}nu) = \textbackslash{}sigma(E) \textbackslash{}cdot n\+\_\+\{\textbackslash{}mathrm\{target\}\} \textbackslash{}cdot l, \textbackslash{}end\{equation\} where (\textbackslash{}sigma(E\+\_\+\textbackslash{}nu)) is the total cross section for the interaction, (n\+\_\+\{\textbackslash{}mathrm\{target\}\}) is the number of targets per unit of volume for such interaction, and (l=40\textbackslash{},m) is the length of the generation volume along the neutrino direction axis. This is the length of the cylinder facing the CCSN. - -\textbackslash{}item Flux Weight\+: \textbackslash{}begin\{equation\} \textbackslash{}label\{eq\+:sn\+\_\+weight\+\_\+flux\} W\+\_\+\{\textbackslash{}mathrm\{flux\}\} = \textbackslash{}frac\{1\}\{N\+\_\+\{\textbackslash{}mathrm\{gen\}\}\} \textbackslash{}cdot \textbackslash{}frac\{r$^\wedge$2\}\{d$^\wedge$2\} \textbackslash{}cdot \textbackslash{}int \textbackslash{}frac\{L(t)\}\{\textbackslash{}bar\{E\}(t)\} dt, \textbackslash{}end\{equation\} where (r=20\textbackslash{},m) is the cylindrical generation volume’s radius, (d) is the distance from Earth where the CCSN is assumed to occur, and (N\+\_\+\{\textbackslash{}mathrm\{gen\}\}) is the number of generated events. - -\textbackslash{}item Effective Weight\+: \textbackslash{}begin\{equation\} \textbackslash{}label\{eq\+:sn\+\_\+weight\+\_\+eff\} W\+\_\+\{\textbackslash{}mathrm\{eff\}\} = N\+\_\+\{\textbackslash{}mathrm\{modules\}\} \textbackslash{}cdot \textbackslash{}frac\{\textbackslash{}bar\{V\}\+\_\+\{\textbackslash{}mathrm\{eff\}\}(m)\}\{V\+\_\+\{\textbackslash{}mathrm\{eff\}\}(m,z\+\_\+\{\textbackslash{}mathrm\{sim\}\})\}, \textbackslash{}end\{equation\} where (N\+\_\+\{\textbackslash{}mathrm\{modules\}\}) is the total modules in the simulated detector, (V\+\_\+\{\textbackslash{}mathrm\{eff\}\}(m, z\+\_\+\{\textbackslash{}mathrm\{sim\}\})) is the effective volume at the simulation depth, and (\textbackslash{}bar\{V\}\+\_\+\{\textbackslash{}mathrm\{eff\}\}(m)) is the mean effective volume for all modules in the detector. The term (m) represents multiplicity, defined as the count of different PMTs within a single module that detected the event within a specific time window. \textbackslash{}end\{itemize\} - -The effective volume can be calculated in different ways. Old simulations of the \mbox{\hyperlink{classm_d_o_m}{m\+DOM}}, described in \href{https://zenodo.org/record/8107177}{\texttt{ this thesis, section 6.\+3}}, were used in past studies. A linear regression of the effective volume concerning the absorption length, derived from various depths, provides each depth\textquotesingle{}s effective volume. Although it is advisable to redo these simulations with a current \mbox{\hyperlink{classm_d_o_m}{m\+DOM}} model, users can temporarily use the old data with a regression line of (V\+\_\+\{\textbackslash{}mathrm\{eff\}\} = b \textbackslash{}cdot x + c), where (x = 1/a) is the inverse of the absorption length. The coefficients (b) and (c), depending on the event\textquotesingle{}s multiplicity, were obtained as follows\+: - -\textbackslash{}begin\{center\} \textbackslash{}begin\{tabular\}\{$\vert$c$\vert$c$\vert$c$\vert$\} \textbackslash{}hline PMTs \& b (slope, units (m$^\wedge$2)) \& c (units (m$^\wedge$3)) \textbackslash{} \textbackslash{}hline 1 \& 15.\+184 \& 0.\+000 \textbackslash{} 2 \& 0.\+135 \& 47.\+005 \textbackslash{} 3 \& 0.\+031 \& 16.\+170 \textbackslash{} 4 \& 0.\+010 \& 8.\+680 \textbackslash{} 5 \& 0.\+004 \& 5.\+105 \textbackslash{} (\textbackslash{}geq6) \& 0.\+003 \& 2.\+909 \textbackslash{} \textbackslash{}hline \textbackslash{}end\{tabular\} \textbackslash{}end\{center\} - -Note that, for more than 5 PMTs, the same fit line is employed due to insufficient statistics at higher PMTs in the effective volume simulation. Additionally, since the absorption length depends on the wavelength, the fits above were obtained assuming a wavelength of (\textbackslash{}lambda = 400\textbackslash{},nm). \doxysubsection*{Files} +Each component is explained as follows\+: \begin{DoxyVerb}- Interaction Probability Weight: + \begin{equation} + \label{eq:sn_weight_int} + W_{\mathrm{int}}(E_\nu) = \sigma(E) \cdot n_{\mathrm{target}} \cdot l, + \end{equation} + where \(\sigma(E_\nu)\) is the total cross section for the interaction, \(n_{\mathrm{target}}\) is the + number of targets per unit of volume for such interaction, and \(l=40\,m\) is the length of the generation + volume along the neutrino direction axis. This is the length of the cylinder facing the CCSN. + +- Flux Weight: + \begin{equation} + \label{eq:sn_weight_flux} + W_{\mathrm{flux}} = \frac{1}{N_{\mathrm{gen}}} \cdot \frac{r^2}{d^2} \cdot \int \frac{L(t)}{\bar{E}(t)} dt, + \end{equation} + where \(r=20\,m\) is the cylindrical generation volume’s radius, \(d\) is the distance from Earth where the + CCSN is assumed to occur, and \(N_{\mathrm{gen}}\) is the number of generated events. + +- Effective Weight: + \begin{equation} + \label{eq:sn_weight_eff} + W_{\mathrm{eff}} = N_{\mathrm{modules}} \cdot \frac{\bar{V}_{\mathrm{eff}}(m)}{V_{\mathrm{eff}}(m,z_{\mathrm{sim}})}, + \end{equation} + where \(N_{\mathrm{modules}}\) is the total modules in the simulated detector, \(V_{\mathrm{eff}}(m, + z_{\mathrm{sim}})\) is the effective volume at the simulation depth, and \(\bar{V}_{\mathrm{eff}}(m)\) is + the mean effective volume for all modules in the detector. The term \(m\) represents multiplicity, defined + as the count of different PMTs within a single module that detected the event within a specific time window. +\end{DoxyVerb} + The effective volume can be calculated in different ways. Old simulations of the \mbox{\hyperlink{classm_d_o_m}{m\+DOM}}, described in \href{https://zenodo.org/record/8107177}{\texttt{ this thesis, section 6.\+3}}, were used in past studies. A linear regression of the effective volume concerning the absorption length, derived from various depths, provides each depth\textquotesingle{}s effective volume. Although it is advisable to redo these simulations with a current \mbox{\hyperlink{classm_d_o_m}{m\+DOM}} model, users can temporarily use the old data with a regression line of $V_{\mathrm{eff}} = b \cdot x + c$, where $x = 1/a$ is the inverse of the absorption length. The coefficients $b$ and $c$, depending on the event\textquotesingle{}s multiplicity, were obtained as follows\+: + +\begin{DoxyVerb}* | multiplicity | b (slope, m^2) | c (m^3) | +* |--------------|----------------------------|------------------| +* | 1 | 15.1843 | 0.000 (imposed)| +* | 2 | 0.1352 | 47.005 | +* | 3 | 0.0306 | 16.170 | +* | 4 | 0.0095 | 8.680 | +* | 5 | 0.0039 | 5.105 | +* | >= 6 | 0.0026 | 2.909 | +* \end{DoxyVerb} + + +Note that, for more than 5 PMTs, the same fit line is employed due to insufficient statistics at higher PMTs in the effective volume simulation. Additionally, since the absorption length depends on the wavelength, the fits above were obtained assuming a wavelength of $\lambda = 400\,nm$. \doxysubsection*{Files} \begin{DoxyCompactItemize} \item file \mbox{\hyperlink{_o_m_sim__supernova_8cc}{OMSim\+\_\+supernova.\+cc}} diff --git a/latex/radioactive__decays_2include_2_o_m_sim_detector_construction_8hh__incl.pdf b/latex/radioactive__decays_2include_2_o_m_sim_detector_construction_8hh__incl.pdf index a001bf85ac..bf74119114 100644 Binary files a/latex/radioactive__decays_2include_2_o_m_sim_detector_construction_8hh__incl.pdf and b/latex/radioactive__decays_2include_2_o_m_sim_detector_construction_8hh__incl.pdf differ diff --git a/latex/radioactive__decays_2include_2_o_m_sim_event_action_8hh__incl.pdf b/latex/radioactive__decays_2include_2_o_m_sim_event_action_8hh__incl.pdf index 9f9921f119..f651c4d004 100644 Binary files a/latex/radioactive__decays_2include_2_o_m_sim_event_action_8hh__incl.pdf and 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  • CADMesh
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  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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  • CADMesh
  • File
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  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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  • CADMesh
  • File
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    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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  • CADMesh
  • File
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    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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diff --git a/struct_decay_stats-members.html b/struct_decay_stats-members.html index 2be9028f04..ac995a5148 100644 --- a/struct_decay_stats-members.html +++ b/struct_decay_stats-members.html @@ -129,7 +129,7 @@ diff --git a/struct_decay_stats.html b/struct_decay_stats.html index f75e382061..fddfc719ee 100644 --- a/struct_decay_stats.html +++ b/struct_decay_stats.html @@ -205,7 +205,7 @@

  • DecayStats
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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diff --git a/struct_evt_stat-members.html b/struct_evt_stat-members.html index c2dcaec5fb..784b90f017 100644 --- a/struct_evt_stat-members.html +++ b/struct_evt_stat-members.html @@ -132,7 +132,7 @@ diff --git a/struct_evt_stat.html b/struct_evt_stat.html index 1081fec823..bd6359527c 100644 --- a/struct_evt_stat.html +++ b/struct_evt_stat.html @@ -273,7 +273,7 @@

  • EvtStat
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
  • Generated on Fri Sep 29 2023 19:57:37 for OMSim by doxygen 1.9.1
diff --git a/struct_global_position-members.html b/struct_global_position-members.html index ec15d69486..0334a60379 100644 --- a/struct_global_position-members.html +++ b/struct_global_position-members.html @@ -129,7 +129,7 @@ diff --git a/struct_global_position.html b/struct_global_position.html index 24624db98d..4f681f0c03 100644 --- a/struct_global_position.html +++ b/struct_global_position.html @@ -201,7 +201,7 @@

  • GlobalPosition
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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diff --git a/struct_hit_stat-members.html b/struct_hit_stat-members.html index 6713d55a1c..77884bdd7c 100644 --- a/struct_hit_stat-members.html +++ b/struct_hit_stat-members.html @@ -135,7 +135,7 @@ diff --git a/struct_hit_stat.html b/struct_hit_stat.html index f59e661580..99205d04b7 100644 --- a/struct_hit_stat.html +++ b/struct_hit_stat.html @@ -321,7 +321,7 @@

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    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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diff --git a/struct_hit_stats-members.html b/struct_hit_stats-members.html index c684ba5ebc..8c5cf253b4 100644 --- a/struct_hit_stats-members.html +++ b/struct_hit_stats-members.html @@ -136,7 +136,7 @@ diff --git a/struct_hit_stats.html b/struct_hit_stats.html index decd6884aa..f1f2880234 100644 --- a/struct_hit_stats.html +++ b/struct_hit_stats.html @@ -326,7 +326,7 @@

  • HitStats
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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diff --git a/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse-members.html b/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse-members.html index 989e2e60da..90a7b7c5de 100644 --- a/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse-members.html +++ b/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse-members.html @@ -128,7 +128,7 @@ diff --git a/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse.html b/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse.html index 9105c71178..ed174b2810 100644 --- a/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse.html +++ b/struct_o_m_sim_p_m_t_response_1_1_p_m_t_pulse.html @@ -188,7 +188,7 @@

  • OMSimPMTResponse
  • PMTPulse
    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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diff --git a/structabc_detector_component_1_1_component-members.html b/structabc_detector_component_1_1_component-members.html index 3741fc0cc0..1573518ee7 100644 --- a/structabc_detector_component_1_1_component-members.html +++ b/structabc_detector_component_1_1_component-members.html @@ -130,7 +130,7 @@ diff --git a/structabc_detector_component_1_1_component.html b/structabc_detector_component_1_1_component.html index 6b456a9872..ec89cf130e 100644 --- a/structabc_detector_component_1_1_component.html +++ b/structabc_detector_component_1_1_component.html @@ -224,7 +224,7 @@

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    • -
  • Generated on Fri Sep 29 2023 19:36:52 for OMSim by doxygen 1.9.1
    • +
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