v00-16-pre
Pre-releasev00-16
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2018-02-22 Dan Protopopescu (PR#201)
- Removed some unused parameters
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2018-02-22 Daniel Jeans (PR#200)
- to ensure that consistent maximum step lengths are used in all models, moved their definition to common directory
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2018-02-27 Daniel Jeans (PR#199)
- implement downstream magnets in ILD models:
- thickened beampipe in regions of final focus magnets
- should reproduce the Mokka models
- currently verifying positions with accel. experts, so details may still change
- implement downstream magnets in ILD models:
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2018-02-26 Andre Sailer (PR#203)
- DDSim: allow passing arbitrary arguments to add_argument, needed for #196 , purely behind the scenes
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2018-02-28 Daniel Jeans (PR#204)
- implement step limits in SEcal06 driver (SEcal06_Helpers.cpp)
- apply cal_limits to ECAL descriptions (barrel, endcap, ECring) in ILD_common_v02
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2018-02-28 Ete Remi (PR#196)
- Added new command line parameters to ddsim
- --eventParameters (list) to write event parameters to every output lcio events
- --runNumberOffset (int) to offset the run number counter in lcio output file
- --eventNumberOffset (int) to offset the event number counter in lcio output file
- Added new command line parameters to ddsim
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2018-02-13 Andre Sailer (PR#197)
- DDSim: Print the startUp and event processing time separately in addition to total runtime
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2017-12-01 TiborILD (PR#186)
- update ILD models w/ SDHcal:
- change the names of original SimCalorimeterHit collections of SDHCAL to the same ones as introduced in hybrid models, i.e. HCalBarrelRPCHits, HCalEndcapRPCHits,HCalECRingRPCHits
- update ILD models w/ SDHcal:
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2017-11-23 Dan Protopopescu (PR#185)
- SiD_o2_v02: Fix BeamCal segmentation (thanks to @shaojunlu), Fixes #184
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2017-11-23 Shaojun Lu (PR#183)
- Update lcgeoTests for ILD to ILD_l5_v02 and ILD_s5_v02.
- the current models for optimisation studies, will be tested during the build.
- Update lcgeoTests for ILD to ILD_l5_v02 and ILD_s5_v02.
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2018-03-16 Frank Gaede (PR#210)
- improve TPCSDAction
- enable writing of TPCSpacePoint and TPCLowPtCollections
- TPCLowPtCollections is only written if
TPCLowPtStepLimit==true
- add steering properties to TPCSDAction
- use in ddsim:
SIM.action.mapActions['tpc'] = ('TPCSDAction', {'TPCLowPtCut': 10*MeV , 'TPCLowPtStepLimit' : True })
- use Mokka default values:
Control.TPCLowPtCut = CLHEP::MeV ; Control.TPCLowPtStepLimit = false ; Control.TPCLowPtMaxHitSeparation = 5. * CLHEP::mm ;
- properly access layerID through IDDescriptor
- improve TPCSDAction
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2018-03-14 Daniel Jeans (PR#209)
- new driver for tube of square cross-section (BoxSupport_o1_v01_geo.cpp)
- new driver for yoke endcaps with square central hole (Yoke06_Endcaps.cpp)
- adjust description of QD0 and first extraction quad, and add its cryostat
- remove more upstream magnets
- include forward region support tubes: around QD0, outer tube froum outside -> LHCAL, and between ecal endcap and ring
- update yoke design to fit with this support structure
- implement the above in the ILD_?5_v02 models
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2017-12-12 Dan Protopopescu (PR#188)
Version 3 of the SiD option 2 model (not final though). Main changes and updates:- cleaned up all XMLs
- using DetIDs
- unified segmentation and cell ID encoding
- added type_flags where missing
- updated plugins
- added envelopes where missing
- stepped design Muon calorimeters use now scintillator instead of RPCs
- merged barrel+endcap envelopes for the Muon calorimeter
- added or updated certain drivers
- included alternate brass HCal
- added common tracker barrel+endcap envelope
- implemented some ECal barrel driver fixes
- checked: no overlaps
- added test_SiD_o2_v03
To check:
- Muon caloData definitions
- ECal towers visibility attributes
- LumiCal and BeamCal envelopes
A detailed table of changes is available in
https://www.evernote.com/l/AJ2Q2yTuLwRGVqYpSNB8HRKx-iBxYQ6Ry0s -
2018-03-05 Frank Gaede (PR#207)
- activate G4StepLimiterPhysics in DDSim by default
- needed to limit the steps in detector volumes and regions
- activate G4StepLimiterPhysics in DDSim by default
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2018-03-05 Dan Protopopescu (PR#202)
Minor corrections to SiD_o2_v03:- Corrected LumiCal grid size parameters
- Added hole in the BeamCal (beam pipe parameters not used with the current driver)
- Removed DetType_AUXILIARY flag from BeamCal
- Removed some unused parameters
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2018-03-28 Frank Gaede (PR#214)
- Fix for the removal of DDSurfaces which have been merged into DDRec
- includes from
DDSurfaces
->DDRec
- namespace
DDSurfaces
->dd4hep::rec
- includes from
- Fix for the removal of DDSurfaces which have been merged into DDRec
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2017-12-11 Oleksandr Viazlo (PR#193)
- new FCCee_o1_v02 detector model
- Material budget of VTX was increased for 50%
- change of LumiCal_cell_size from 1.0 to 1.81 mm, change of LumiCall offset
- add test for FCCee_o1_v02 model, remove test for FCCee_o1_v01
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2017-12-04 Andre Sailer (PR#189)
- Add CLIC_o3_v14 with fixed LumiCal segmentation
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2017-12-04 Frank Gaede (PR#187)
- Set DDSim defaults to Geant4 defaults and retain
largest_step = 10 * m
as recommended in the Geant4 manual (~ detector size). This improves simulation time for single muons approximately a factor 2 and for single pi+ for 25%
- Set DDSim defaults to Geant4 defaults and retain
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2018-03-27 Ete Remi (PR#213)
- DD4hepSimulation:
- Fixed division by zero when no event has been processed, Fixes #208
- DD4hepSimulation:
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2018-03-22 Oleksandr Viazlo (PR#211)
- create FCCee_dev detector model (extended ECAL endcap, shrinked HCAL ring, reduced magnetic field in yoke from 1.5 T to 1.0 T)
- add test for the model
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2018-03-23 Daniel Jeans (PR#212)
- writeAllILDCompactDescriptions.py: python script to create compact detector descriptions with different variations: large/small, ideal/realistic fields at 250/500 GeV, with or without anti-DID fields, different reconstruction options
- compact descriptions all kept in one directory ILD_sl5_v02
- each model is linked individually
- some models are not yet functional: in particular small models with realistic fields, for which no field maps are yet available. [ ie ILD_s5_v03, v04, v05, v06 ]
- ILD_?5_v02 models and their options should be completely unchanged