Kamil Sedlak
db7b6a80f4
Added geometric shape "BarWithBevelledEdgesX" used for Alexey's investigation of light transport throuhg a scintillator bar. This version is done before implementing changes made by James Lord
1229 lines
77 KiB
Plaintext
1229 lines
77 KiB
Plaintext
musr_X.root:
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X=
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==============================================================================================
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Microbeam - Alex & Elvezio, April 2012
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260034 ... ideal parallel beam, middle collimator 1mm, sample collimator 0.1mm
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260033 ... ideal parallel beam, middle collimator 10mm, sample collimator 1mm
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260032 ... ideal parallel beam, middle collimator 1mm
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260031 ... ideal parallel beam, middle collimator 10mm
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260024 ... FOR075_microbeam.DAT, middle collimator 1mm, sample collimator 0.1mm
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260023 ... FOR075_microbeam.DAT, middle collimator 10mm, sample collimator 1mm
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260022 ... FOR075_microbeam.DAT, middle collimator 1mm
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260021 ... FOR075_microbeam.DAT, middle collimator 10mm
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260008-9 ... files for tuning the quadrupole triplets using the "optimize.py" python script
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260001 ... first trial
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==============================================================================================
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NEUTRON DETECTOR - Alexey, November 2011:
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250001 - first tests for a neutron detector
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==============================================================================================
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GPS
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5018? ... like 5013? but with the new (pyramidal) forward veto - a short one
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5017? ... like 5013? but with the new (pyramidal) forward veto - a middle one
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5016? ... like 5013? but with the new (pyramidal) forward veto - a long one
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5013? ... like 50111 (but larger statistics)
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5012? ... like 50110 (but larger statistics)
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50111 ... like 50081 but after geometry bug corrected (new geometry)
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50110 ... like 50089 but after geometry bug corrected (old geometry)
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CORRECTED BUG IN THE GEOMETRY (FOUND BY ALEX AMATO) 1.2.2012
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50108 ... like 50102, old geometry
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50107 ... like 50101, old geometry
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50102 ... like 50101, 150G
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50101 ... based on 50081 but with the longitudinal polarisatoin, 50G
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50091-93 ... like 50071-73 but with Geant4.9.5 (13.1.2012)
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50090 ... like 50081 but with the old geometry
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50089 ... like 50081 but with the old geometry (repetition of the 50021 geometry)
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50081-83 ... like 50061-63 but with Geant4.9.5 (13.1.2012)
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50080 ... like 50081 but at 0 magnetic field
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50071-73 ... like 50051-50053 but with the new GPS design from 9.12.2011
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50061-63 ... like 50021-50023 but with the new GPS design from 9.12.2011
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50051 ... like 50021 but more focused beam; some detectors have different numbers!!!
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50023 ... like 50021 but B=0.5 T
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50022 ... like 50021 but B=0.05 T
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50021 ... old GPS geometry, wide beam, B=0.005 T
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50001 ... GPS geometry
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==============================================================================================
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GPD
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40171 ... like 40111, but with larger angular coverage by another 2 "backward" detectors.
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40161,2 ... like 40121, but the collimator is thicker only in the insert region of 2x4cm.
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40152 ... like 40111 but with collimator 2 shifted: -25cm -> -45cm
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40151 ... like 40111 but with collimator 2 shifted: -25cm -> -35cm
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40141-3 ... like 40111-3 but with both lead collimators thicker
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40131-3 ... like 40111-3 but with collimator at 25cm made thicker
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40127 ... like 40123 but with m-counter embedded inside another veto detector
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40126 ... like 40123 but with a narrow active collimator (to apply it in anticoincidence with backw. counters)
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40125 ... like 40123 but with smaller opening in active collimator
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40124 ... like 40123 but with larger m-counter
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40121-3 ... like 40111-3 but with collimator at 10cm made thicker (3cm -> 5cm)
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40113 ... like 40111 but GPDcollimator removed and added scintillators 21 and 22
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Al plate made of scintillator (veto counter)
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... i.e. like 40106 (40093)
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40112 ... like 40111 but with GPDcollimator made of Pb (instead of Cu)
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40111 ... like 40063 but with Geant4.9.4 (9.2.2011), 8000000 events
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40106 ... like 40093 but with Geant4.9.4 (31.1.2011) less events than 40105
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40105 ... like 40093 but with Geant4.9.4 (28.1.2011)
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40104 ... like 40103 but GPDcollimator made of Pb (instead of Cu)
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40103 ... like 40101 but scintillators 21 and 22 removed and GPDcollimator returned back
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-> i.e. this run should be very close to 40063 but with thicker GPDcollimator2 collim
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40102 ... like 40101 but scintillators 21 and 22 removed (probably not very interesting run)
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40101 ... like 40093 but with GPDcollimator2 made thicker (3cm -> 5cm)
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40093 ... like 40063 but GPDcollimator removed and added scintillators 21 and 22
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Al plate made of scintillator (veto counter)
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40082 ... like 40063 but GPDcollimator made of Pb
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40081 ... like 40063 but thicker GPDcollimator
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40061-2 ... SetLargestAcceptableStep=200, beam according to measurement
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done by Alexander with the camera
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40051-2 ... test runs without detector to see where the muons stop in sample plane
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40041-5 ... significantly improved geometry
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40033 ... 0.03T, vertexsigma 5mm, p=100.0 +- 3 MeV
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40032 ... 0.03T, vertexsigma 5mm, p=100.0 +- 0 MeV
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40031 ... OT, vertexsigma 5mm, p=100.0 +- 0 MeV
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40030 ... OT, vertexsigma 0mm, p=100.0 +- 0 MeV
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40001 ... initial GPD design
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===============================================================================================
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Dec 2011 tests of Hight Field
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31044 ... similar to 31035 but at B= 50 gauss
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31043 ... similar to 31035 but at B=500 gauss
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31042 ... similar to 31035 but at B= 50 gauss and without the second collimator "collimatorA2"
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31041 ... similar to 31035 but at B=500 gauss and without the second collimator "collimatorA2"
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May 2011 tests of High Field
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31036 ... like 31035 but B=8.0T.
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31035 ... 10M, B=0.5T, improved geometry (Ti windows, Kapton window, sample holder)
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31006 ... large stat. simulation, B=8.0T
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31005 ... large stat. simulation, B=0.5T
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31004 ... large stat. simulation, B=50G
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31003 ... large stat. simulation, B=0T.
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31002 ... modified beam pipe; field rising from 0 to 10 T
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31001 ... first tests to see the dependence of muon rate on field
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===============================================================================================
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Dec 2010 test of High Field
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30711-36 ... large statistics simulation like 30605 and other fields
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306?? ... using 2 adjacent detector segments (more statistics than 304?? and a small bug in *.mac corrected)
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30583 ... like 30582, but with the goulombRegion commented out
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30582 ... like 30581, but with the test size of positron counters
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30581 ... like 30580, but with the ALC fieldmap
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30580 ... like 8805
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30512-3 ... using all 8 segments of detectors
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304?? ... using 2 adjacent detector segments
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30220-5 ... like 30200-5 but with longitudinal muon polarisation
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30200-5 ... like 30100-5 but with TURTLE beam
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30100-5 ... December 2009 test for the High Field instrument done in ALC area - point-like beam ; transverse spin polaris.
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==================================================================================================
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SPIN ROTATOR STUDY
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20810 ... like 20661 but after the bug correction
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20809 ... like 20641 but after the bug correction
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20808 ... like 20611 but after the bug correction
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20807 ... like 20612 but after the bug correction
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20806 ... like 20501 but after the bug correction
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20805 ... like 20502 but after the bug correction
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20804 ... like 20503 but after the bug correction
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20803 ... like 20504 but after the bug correction
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20802 ... like 20505 but after the bug correction
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20801 ... like 20511 but after the bug correction
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6.9.2010 - bug found and corrected in the field-map extrapolation of the electric and magnetic fields
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for the spin-rotator (3DEOpera and 3D and symmetryType=1 or 2).
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20709 ... like 20708, but with R1IN and R1OU shifted, and beam starting just at spinrot entrance.
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20708 ... like 20702, but without the windows
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20707 ... like 20702, p=28.0 MeV/c.
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20706 ... like 20702, p=27.8 MeV/c.
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20705 ... like 20702, p=27.6 MeV/c.
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20704 ... like 20702, p=27.2 MeV/c.
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20703 ... like 20702, p=27.0 MeV/c.
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20702 ... like 20701 but with parallel and monoenergetic beam (27.4 MeV/c)
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20701 ... repetition of 20661 but with Geant 4.9.4.p02 (24.8.2011)
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20391-4...like 20361-4 but without muon decays
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20381 ... like 20351 but without muon decays
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20371 ... like 20321 but without muon decays
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20361 ... like 20351 but with monoenergetic beam
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20351 ... like 20321 but with the matched B and E fields according to the calculation (calculations for 27.4 MeV/c muons)
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20331 ... like 20321 but with uniform B and E fields
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20321 ... repetition of 20313
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20311-6 ... based on 20303 and 20211 using the newest TURTLE (from February 2010)
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20303 ... like 20181 but using Geant4.9.3 with appropriately modified steering file
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20302 ... repeating 20181 but (i.e. using Geant4.9.p02)
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20301 ... like 20181 but using Geant4.9.3
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2023? ... like 20181 but using NEW VERSION OF TURTLE
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2022? ... like 2021? but with the turtle file generated using NEW VERSION OF TURTLE
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2021? ... like 2020? but with larger gap in between the magnets of the spin rotators
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2020? ... like 20181 but with correction of "/gun/vertex 0 0 -12032 mm" and different "/gun/turtleInterpretAxes"
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2019? ... like 2018? but vith v04 instead of b05c
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2018? ... like 2013? but with a little bit larger e01
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2016? ... like 20131 but with varying QSE4
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2015? ... like 2013? but with /gun/turtleInterpretAxes x-y
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2014? ... electrodes = e01, magnetic field = v04, Turtle = reggiani_Jan2010_z-12032, varying e01
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2013? ... electrodes = e01, magnetic field = b05c, Turtle = reggiani_Jan2010_z-12032, varying e01
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2012? ... electrodes = e01, magnetic field = b05c, Turtle = pie3_HiField_d05_x30_z-15111
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2011? ... electrodes = e01, magnetic field = v04, Turtle = pie3_HiField_d05_x30_z-15111
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20024 ... like 20023 but with y coordinate interpreted as -y
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20023 ... like 20021 but with E and B fields negative
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20022 ... like 20021 but with y coordinate interpreted as -y
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20021 ... Spin Rotator study - using output from TURTLE generated just in front of the spin rotator
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==================================================================================================
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HIGH FIELD
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14602-12 ... based on 14601 (generated by perl script), but varying the sample (and also cryostat) position.
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All at 1 T field.
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14601 ... based on 14600, but with wide TURTLE beam, and with some modifications in the detector numbering
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(to be closer to my earlier numbering). Field of 1T.
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14600 ... file from J. Rodrigez (ALC-modified flow cryostat)
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14593-4 ... like 14591-2 but with point-like beam.
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14592 ... like 14591 but 10M events and only interesting events saved
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14591 ... like 145?? but with longitudinal polarisation, field only 50 Gaus (transvers.)
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--> Robert wants to know the long. ampl. of asymm.
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145?? ... like 144??, but all events saved and statistics only 1M.
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1448? ... like 14452 but very large statistics
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144?? ... based on 14060; updated geometry according to the latest knowledge; 8+1 validation counters
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143?? ... 28.3.2012 quick (dirthy) test with flow cryostat requested by Robert - using the 0.4 mm Cu shield
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142?? ... 28.3.2012 quick (dirthy) test with flow cryostat requested by Robert - using the 1.0 mm Al shield
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141?? ... like 140?? but with TURTLE with zero momentum bite
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14020 ... like 14010 but smaller statistics and storing all events (not just the ones with hit).
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14001 ... 15.3.2012; Geant 4.9.5; based on 12700 and 31043
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-----
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13850-61 ... like 13750 but with the M-counter as in 12700
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13750-61 ... like 13550 but with the old beamline+old collimators (12250) shifted 9mm upstream.
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13650-61 ... like 12250 (repetition to see whether I can reproduce 12250).
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13550-61 ... like 13150 but with the modified M-counter region and the old beamline+old collimators (12250).
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13450-61 ... like 12260 but with the beamline and collimators as in 12950.
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13350-61 ... like 13250 but with both collimators as in 12260 (just on different place).
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13250-61 ... like 13150 but with the old (first) collimator (as in 12260).
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13150-61 ... like 12950 but using 400 mum M-counter (300 mum in previous runs)
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13050-61 ... like 12950 but using 400 mum M-counter (300 mum in previous runs) - bug (M0 overlap)
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12950-61 ... like 12700 but using smaller sample holder (diameter=3mm instead of 8mm)
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12800-61 ... like 12700 but using larger sample (8mm diameter instead of 5mm diameter)
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12700-61 ... NEW DR geometry (based on status of 26.8.2011) (geometry started from runs 12360+30711)
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12400-61 ... like 12300 but with TURTLE with zero momentum bite
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12300-61 ... based on 8800, but with the different magnet and Turtle files (flow cryostat)
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12200-61 ... like 12100 but with Geant4.9.4.p02
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12199 ... like 12160 but with Geant4.9.4 (28.1.2011)
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12149 ... like 12110 but with Geant4.9.4 (28.1.2011)
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12000-11 ... like 10900-10911 but with Geant 4.9.3 and with a new Turtle file (FOR077_reggiani_Feb2010.dat)
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11650-9 ... Geant 4.9.3 using Coulomb scattering for muons (16.3.2010)
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11631-5 ... different parameters of the processes in Geant 4.9.3. Problem with generated nr of muons
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due to a bad compilation on merlin00 (effects triggered/generated rate, should
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not cause other problems) (15.3.2010)
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116?? ... like 109?? but with Geant 4.9.3, however not modifying the processes (i.e. processes as in 4.9.2.p02 *.mac files)
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115?? ... high statistics, old TURTLE Geant 4.9.3
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114?? ... like 109?? but with February TURTLE (new turtle executable) and Geant 4.9.3 and 12M of events
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113?? ... like 109?? but with January TURTLE (new turtle executable) and Geant 4.9.3
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11210 ... like 11110 but with Geant 4.9.3
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111?? ... like 109?? but with the NEW TURTLE file from Davide using the NEW TURTLE executable
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110?? ... like 109?? but with the newest Cryogenics magnet (from 30.11.2009)
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109?? ... like 106?? but with the newest OI magnet (from 3.11.2009)
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108?? ... like 106?? but with the longitudinal field (also OK for the pile-up background study)
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107?? ... like 106?? but with the field rotation
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106?? ... like 102??, but without any field rotation and using new TURTLE file from Davide (pie3_HiField_d05_x30.dat)
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105?? ... like 104?? ... (generated beam) but without the rotation of the magnet
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10420 ... like 10410 but with magnetic field made positive instead of negative. 10420 and 10410 are expected to be
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identical, if difference found, would be very strange!
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104?? ... like 102?? but with the generated beam (instead of Turtle) with tiltsigma and pitch.
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10330-41 ... like 10310-11 but only 5mrad rotation
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10310-11 ... like 10210 but with the different directions of the field map rotation (to find out "the worst case scenario")
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(5mrad rotation)
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102?? ... like 98?? but with the negative field map (to have the same field map sign as in the old OI map)
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101?? ... repetition of 91??
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10017-10021 ... like 10007 - 10011 but with the field map rotated in oposit direction (should not change anything)
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100?? ... like 97?? but with musrSim and field of the solenoid tilted by 5 mrad
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99?? ... like 97?? but with musrSim and field of the solenoid tilted by 20 mrad
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98?? ... like 97?? but with musrSim and field of the solenoid tilted by 10 mrad
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97?? ... like 85?? but with the new magnet OI_082009
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96?? ... like 87?? but with musrSim and field of the solenoid tilted by 20 mrad
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95?? ... like 87?? but with musrSim and field of the solenoid tilted by 10 mrad
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94?? ... like 85?? but with musrSim and field of the solenoid tilted by 20 mrad
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93?? ... like 85?? but with musrSim and field of the solenoid tilted by 40 mrad
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92?? ... like 85?? but with musrSim and field of the solenoid tilted by 100 mrad
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91?? ... like 85?? but with musrSim and field of the solenoid tilted by 10 mrad
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90?? ... like 88?? but using the merged code (musrSim)
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8900-11,50-61 ... design of Alexey's dilution cryostat
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8800-11,50-61 ... like 7600 but with massiver collimators (small flow cryostat) + sample holder
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8700-11,50-61 ... like 8000 but with massiver collimators (56 mm cryostat)
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8600-11,50-61 ... like 84?? but with massiver collimators
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8500-11,50-61 ... like 8333 = new suggestion from Robert + more massive collimators
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8450-61 ... pileup for 8400_11
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8400-11 ... small dilution cryostat (new suggestion from Robert) but using the veto + veto plate a'la Elvezio
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8350-61 ... pileup for 8300_11
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8300-11 ... small dilution cryostat (new suggestion from Robert)
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8250-61 ... pileup for 8200_11
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8200-11 ... like 8100-10 but using Elvezio's idea of veto cylinder (no veto behind the sample!)
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8150-61 ... pileup for 8100_11
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8100-11 ... like 8000-10 but for 48 mm dilution cryostat
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8050-61 ... pileup for 8000_11
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8000-11 ... 56 mm dilution cryostat + small active collimator size + sample holder rod + 4 cryostat walls
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7700-11 ... like 7600-11 but for pileup
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7600-11 ... like 7500-11 but with small active collimator size
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7590-96 ... different outer radius of the active collimator
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7520-40 ... like 7500-11 but with fine step in magnetic field
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7500-11 ... like 7400-11 but for the pile-up
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7417 ... like 7405 but with the passive collimator made active (in order to investigate why so many muons stop
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in the M0)
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7400-11 ... similar to 7180-91 (old version of GEANT = 4.9.1.p03, but not with the changes by Gumplinger) with:
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1) Veto cylinder 2mm thick, with 0.5mm gap around wals, and veto + cylinder combined together
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2) 1 mm Al plate around M0
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3) Larger windows in cryostat flanges, one of them changed from Ti to Mylar
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7300-11 ... like 7180-91 but with new GEANT version 4.9.2
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7250-61 ... like 7221 (detector radius 50mm) but for fields between 0 and 10 T
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7230-41 ... like 7222 (detector radius 60mm) but for fields between 0 and 10 T.
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7220-02 ... like 7190 (at 9.99 T) but with larger inner detector radius (40, 50 and 60 mm) (+ modified Active Collim. to fit in pos. counters)
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7200-11 ... like 7180-91 but with smaller m0 counter (3 mm instead of 6mm in diameter)
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7198 ... Robert's independent test using unpolarised muons (to see that the asymmetry amplitude is zero)
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7180-91 ... corrected 7160-71 but with an 8 mm gap between active collimator and the positron detector,
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and only a half veto cylinder (forward half removed), and thinner veto (2mm instead of 2.4mm),
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and larger m0 counter (6 mm instead of 3 mm in diameter)
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7160-71 ... like 7140-50 but with the short cryostat, but with an conflict in geometry (veto cylinder goes through
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cryostat window).
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7140-50 ... like 6720-30 but with the flange on the cryostat 1 outside the cylinder
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7120-30 ... like 6720-30 but with a box-like 10T field in the volume of 15x10cm around the sample (z=15cm, R=10cm).
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7100-10 ... like 6720-30 but with JASTEC field map
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70?? ... like 69?? but for the pileup background (no event reweighting, decay times -1 -1)
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6900-90 ... like 6720-30 but for different magnets: 2420d, 2420e, alc_kamil_2D, worsened_A_OI_10T_grid_xz, ISIS
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68?? ... like 67?? but for the pileup background (no event reweighting, decay times -1 -1)
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6760-70 ... like 6720-30 but with FOR077_pie3_HiField_d02_x15.dat and correct distnace (1.3 meters) from the sample!!!
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6740-50 ... like 6720-30 but with FOR077_pie3_HiField_d01_x15.dat and correct distnace (2.5 meters) from the sample!!!
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6720-30 ... repeating 6020-30 with musr_Gumplinger_and_Apos executable
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6670,6690 ... like 6630 and 6650 but with no limit on muon decay time and all events saved (for the pile-up investigations)
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6630,6650 ... like 6530 and 6550 but with new (longer) turtle files from Davide and without any event reweighting
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6560, 61, 70 ... like 6540,41,50 but with larger TURTLE input file and musr_Gumplinger_and_Apos executable
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6540-50 ... like 6020-30 but for the new turtle input file (focused beam) from Davide FOR077_pie3_HiField_d02_x15.dat
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6520-30 ... like 6020-30 but for the new turtle input file (parallel beam) from Davide FOR077_pie3_HiField_d01_x15.dat
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63?? ... for the pile-up background (shound not be done with event reweighting next time!)
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...
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...
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6020-30 ... (2008.11. ) ... like 6000-10 but with additional cylindrical veto counter.
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6000-10 ... (2008.11. ) ... cryostat with 30mm outer diameter, 3 walls
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5900-10 ... (2008.11.05) ... like 5500-10 but with 60mm diameter detector (dilution-like cryostat).
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5800-10 ... (2008.10.24) ... like 5500-10 but with the ISIS magnet
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5700-10 ... (2008.10.24) ... like 5500-10 but with the ALC magnet
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==== 2008.10.24 ======
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FOR070_2008_09_29_XXII.DAT: RMS of x_ini(z=-1.0m) = 35-40 mm; RMS of y_ini(z=-1.0m) = 27-30 mm;
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boundary R=70mm;
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p_ini = 27.74 +/- 0.72 MeV/c; p_min_allowed=25.2, p_max_allowed=29.8.
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==== 2008.10.21 ==== change on Merlin00 - for some reason musr executable crashes now
|
|
5600-10 ... like 5500-10 but with the Cryogenics magnet
|
|
5540-50 ... (2008.11.05) like 5500-10 but with larger detector and cryostat (inner detector diameter = 40mm).
|
|
The size of veto counter is the same as in 5520-30, larger than in 5500-5510.
|
|
5520-30 ... like 5500-10 but with larger detector, cryostat and veto counter (inner detector diameter = 30mm)
|
|
5500-10 ... like 5370-80 but with FOR070_2008_09_29_XXII.DAT turtle file (broader momentum bite)
|
|
==== some changes in the code
|
|
5370-80 ... like 5350-60 but with FOR070_2008_09_29_XII.DAT turtle file
|
|
5350-60 ... 2 milion of events, 0-10T field, FOR070_2008_09_29_XI.DAT turgle file, OI magnet
|
|
5220-30
|
|
5200-10
|
|
5182 ... 3 milion of events with APDs at 0 T field
|
|
5181+3 ... 2 and 1 milion of events with APDs (for radiation studies) at 10 T
|
|
5170-80
|
|
5161-2 ... for Alexey - test of the solid angle of the detector and APD's in 10T and 0T.
|
|
5150-60 ... like 5144 but with FOR070_2008_09_29_I.DAT turtle input file (focused to z=0 at B=0) and B from 0 to 10 T
|
|
5145 ... like 5181 but with 50cm long narrow-part beam-pipe and newly positioned conical collimators
|
|
5143 ... like 5181 but with 50cm long narrow-part beam-pipe
|
|
5142 ... like 5181 (should be exactly the same as 5181)
|
|
5141 ... like 5181 but with ALC-like beam pipe
|
|
====2008.09.29 ==== 1) implementing G4cons (for conical collimators)
|
|
2) numberOfGeneratedEvents in G4PrimaryGeneratorAction (i.e. number of the generated events;
|
|
in case of Turtle nr. of events tried);
|
|
====2008.09.25 ==== just a minor change in program - typeOfProcess variable removed from musrParameters.cc and other routines
|
|
+ steering file restructured
|
|
5139 ... ISIS high field magnet;
|
|
5132-6 ... like 5081 but with field homogeneity worsened 10 times around 10 Tesla; decay times aroud 0.4, 5.4, 10.4, 20.4 and 30.4 microseconds.
|
|
5131 ... like 5081 but with 16 detectors instead of 8.
|
|
5121-4 ... like 5081 but with sigma(p) of 0, 1, 2 and 4 %. (5081 = 3%)
|
|
5110-20 ... like 5083 (i.e. with the Robert's TURTLE input file) and field from 0 to 10 T in steps of 1T.
|
|
5081, 5091-6 ... repeated once again for the updated version of the program
|
|
====2008.09.18.===
|
|
1) Adding the possibility to store the muon polarisation and time
|
|
when first hit occurred in the detector called M0, M1 and M2.
|
|
It is done in a way very similar to "Target" detector.
|
|
2) Nr. of really generated events and the run number is now
|
|
stored into the "geantParameters" vector.
|
|
3) Definitively removed variables "globalTime" and "fieldValue"
|
|
from the root tree.
|
|
5100-7 ... like 5081, 5091-7 but with 2T field in the sample region instead of 10T (but 10T field around the sample)
|
|
replaced 5091-7 ... like 5081 but with the M0-sample distance of 40, 60, 80, 100, 120, 150, 200 mm (instead of 22 mm)
|
|
5085 ... like 5081 but with the 5 T field inside the sample (10 T outside) and M0-sample distance only 7mm (instead of 22mm).
|
|
5084 ... like 5081 but with the 5 T field inside the sample (10 T outside)
|
|
5083 ... like 5081 but with the Robert's TURTLE
|
|
5082 ... like 5081 but with my TURTLE
|
|
replaced 5081 ... similar to 5002 but with 2.4 mm thick veto detector and broather initial beam
|
|
=====2008.09.10==== Some further small improvements
|
|
5067 ... like 5061 but using Coulomb scattering in a G4Region for e+ and e- 8.54 11.51
|
|
5066 ... like 5061 but with Vvv info commented out. 5.04 7.30
|
|
5065 ... like 5061 but with goulombRegion commented out. 8.94 11.60
|
|
5064 ... like 5062 but with the decay times around 100400 ns. 9.25 12.05
|
|
5063 ... like 5061 but seting production cuts in G4Region 5.04 7.39
|
|
5062 ... like 5061 but using Coulomb scattering in a G4Region for muons 9.27 11.82
|
|
5061 ... should be very close to 5041.mac (after the modifications) 8.93 11.59
|
|
=====2008.08.28==== Processes have to be defined in the steering file now.
|
|
G4Region implemented ==> Should allow to define coulomb scattering within G4Region
|
|
==> Should allow to set the production cuts in a G4Region
|
|
5042-52 ... like 5031 but with the decay times around 20400 40400 60400 80400 100400 150400 200400 250400 300400 400400 500400 ns.
|
|
5041 ... like 5031 after the change of code (no difference between 5031 expected)
|
|
=====2008.08.20==== 1) Change in event reweighting ===> The criterium is where the muon decays (and not
|
|
through which volumes it penetrates)
|
|
2) Cleaning of the musrStepingAction.cc code
|
|
5032-4 ... like 5031 but with the decay times around 1400, 10400 and 100400 ns.
|
|
5031 ... like 5002 but after the bug in G4DecayWithSpin was removed (2008.08.19)
|
|
=====2008.08.19==== Bug removed in G4DecayWithSpin causing that there was amplitude dumping as a function of time
|
|
5022 ... like 5002 but with 2.4 mm thick veto detector
|
|
|
|
5020 ... 100k events, decay time fixed to 100405 ns, muons generated at rest inside sample.
|
|
5019 ... like 5009 but with the decay times around 100000400 ns
|
|
5018 ... like 5009 but with the decay times around 10000400 ns
|
|
5017 ... like 5016 but with no muon beam momentum smearing.
|
|
5016 ... test run like 5015 but with decay time fixed to 100405 ns.
|
|
5015 ... like 5009 but just for testing
|
|
5014 ... like 5002 but with M0 counter 200mu thick (instead of 400)
|
|
5013 ... like 5002 but with momentum bite 2 times smaller than in 5002
|
|
5012 ... like 5002 but with the decay times around 1000400 ns
|
|
5010-11 ... like 5002 but with the distance between sample and M0 counter 7 and 12 mm (instead of 22 mm)
|
|
5007-9 ... like 5002, but with the decay times around 1400, 10400 and 100400 ns.
|
|
5006 ... like 5002, momentum bite of sigma 2 times larger than in 5002
|
|
5005 ... like 5002, d=30mm
|
|
5004 ... like 5002, d=24mm
|
|
5003 ... like 5002, d=14mm
|
|
5002 ... like 5001 but high stat. d = 20mm
|
|
5001 ... based on 1351 but with thiner scintillator boxes (low statistics)
|
|
|
|
|
|
|
|
|
|
3200 ... (27.4.2010) like 3048 but with GEANT 4.9.3 (visualisation for the new publication)
|
|
3121 ... (5.10.2009) like 3120 but with only 25 mum thick sampleCellWindow (instead of 50 mum).
|
|
3120 ... (5.10.2009) like 3107 but with: 1) Reduced step lenght of muons to 0.01 mm
|
|
2) Added M0 counter (300 mum of scintillator + 25 mum of Mylar)
|
|
3112 ... like 3111 but with parallel beam
|
|
3111 ... like 3106 but with additional Cu collimator (close to sample, opening of 15mm in diameter)
|
|
3108 ... like 3106 but without the cryostat (Alexey was interested what is the effect of cryostat on asymmetry)
|
|
3107 ... like 3100 with the Cu sample cell filled with water with TURTLE from Davide
|
|
3106 ... like 3100 with the Al sample cell filled with water with TURTLE from Davide
|
|
3105 ... like 3100 with the Cu sample plate with TURTLE from Davide
|
|
3103 ... like 3100 with the Cu sample cell filled with water
|
|
3102 ... like 3100 with the Al sample cell filled with water
|
|
3101 ... like 3100 with the Cu sample plate
|
|
3100 ... like 3027 but with the new ALC cryostat - drawings from Alexey. Test setup. (27.8.2009)
|
|
---
|
|
3068 ... like 3048 but with the new ALC field map form Oleg Kiselev ALC_2D_analytical_oleg.dat
|
|
3067 ... like 3048 but with some variables commented out and with the mean momentum of 26MeV
|
|
3066 ... like 3048 but with some variables commented out and with the mean momentum of 27MeV
|
|
3065 ... like 3048 but with some variables commented out and with the momentum smearing of 3MeV
|
|
3060-2 ... like 3051 but 3.33333333xstatistics in each run
|
|
3055-9 ... like 3050 but 2xstatistics in each run
|
|
3052-4 ... like 3049 but 3.33333333xstatistics in each run
|
|
3049-51 ... like 3048 but with 3 different TURTLE input files
|
|
3048 ... (7.10.2009) like 3043, small step size also for kapton (not only for target)
|
|
3047 ... (9.9.2009) like 3044 but after implementing muTargetMomZ (and smaller statistics)
|
|
3046 ... like 3027 but with muon momentum of 26 MeV
|
|
3045 ... like 3027 but with muon momentum of 27 MeV
|
|
3044 ... like 3027 but with muon momentum smearing of 3 MeV
|
|
3043 ... like 3027 but with no shield-like volumes to allow for positron annihilation
|
|
---
|
|
3042 ... like 3021 but with shifted sample by -2mm
|
|
3041 ... like 3021 but with shifted sample by +2mm
|
|
3040 ... like 3021 but with shifted ALC field by 5cm (centre of the field is at -5.02 cm)
|
|
3039 ... like 3021 but with sample thickness of 1.2 mm
|
|
3038 ... like 3021 but with shifted ALC field by 5cm (centre of the field is at +5.02 cm)
|
|
3037 ... should be (almost) identical 3021
|
|
3036 ... like 3021 but with tilted ALC field by 0.3 deg
|
|
3035 ... like 3021 but with tilted ALC field by 1 deg
|
|
3034 ... like 2021 but with sample thickness only 0.8 mm
|
|
3033 ... like 2021 but with tilted ALC field by 4 deg
|
|
3032 ... like 2021 but with tilted sample by 4 deg
|
|
3031 ... like 2021 but with tilted sample by 1 deg
|
|
3028 ... like 3027 but with step limit in the sample holder of 0.01 mm (for muons and e+, e-)
|
|
3027 ... like 3021 but with step limit in the sample of 0.01 mm (for muons and e+, e-).
|
|
3026 ... like 3023 but with G4MuPairProduction & G4MuBremsstrahlung & G4MultipleScattering off
|
|
3025 ... like 3023 but with G4MuPairProduction & G4MuBremsstrahlung off
|
|
3024 ... like 3023 but with G4MuPairProduction off
|
|
3023 ... like 3021 but with monoenergetic muon beam
|
|
3022 ... like 3021 but with negative muons (mu-) - the difference in low energy treatment of e+ and e- !!!
|
|
3021 ... like 3001 but with sensitive target & all Root varibles stored &
|
|
field volume has ID number 98 (not 99 as target) & new version of musrSim (after implementing
|
|
negative muons).
|
|
3006 ... like 3002 but with negative muons (mu-) - the difference in low energy treatment of e+ and e- !!!
|
|
3005 ... like 3002 but with G4MuPairProduction & G4MuBremsstrahlung & G4MultipleScattering off
|
|
3004 ... like 3002 but with G4MuPairProduction & G4MuBremsstrahlung off
|
|
3003 ... like 3002 but with G4MuPairProduction off
|
|
3002 ... like 3001 but with fewer setps in field (less events), sensitive target & all Root varibles stored &
|
|
field volume has ID number 98 (not 99 as target)
|
|
3001 ... like 2511 but with musrSim (2009-05-27)
|
|
2921 ... (2008.10.28) like 2201 but after many many modifications in the program
|
|
=== 2008.10.28 ========================
|
|
2901-05 ... like 2511 but with coulomb scattering in target (for both e+ and mu+) and 1/5 statistics
|
|
|
|
2621-05 ... like 2601-05 but with TURTLE file ...*KAMIL*...
|
|
2601-05 ... mass production: like 2511 but with the TURTLE file FOR061_2008_04_22.DAT
|
|
2591-95 ... mass production: like 2511 but with the point-like beam (/gun/vertexsigma 0 0 0 mm)
|
|
2581-85 ... mass production: like 2511 but with the homogeneous beam (/gun/vertexsigma -20 -20 0 mm)
|
|
2571-75 ... mass production: like 2511 but with the 28+-3 MeV muon beam
|
|
2561-65 ... mass production: like 2511 but with the 26 MeV muon beam
|
|
2551-55 ... mass production: like 2511 but with the 27 MeV muon beam
|
|
2541-45 ... mass production: like 2511 but with the 3mm sample and 1mm Pb shield
|
|
2531-35 ... mass production: like 2511 but with the 3mm sample
|
|
2521-25 ... mass production: like 2511 but with the 1mm Pb shield
|
|
2511-15 ... mass production: basic distribution, similar to 2501 but with a tiny change in the sample holder
|
|
2504 ... like 2501 but with the 3mm sample and 1mm Pb shield
|
|
2503 ... like 2501 but with the 3mm sample
|
|
2502 ... like 2501 but with the 1mm Pb shield
|
|
2501 ... new default; like 2500 but with less variables stored
|
|
2500 ... like 2178 (but with the corrected GlobalField implementation):
|
|
p=28MeV; Kapton; det_particleID added;
|
|
new field from Toni; polarisation =95%; all variables stored
|
|
|
|
2425 ... like 2422 but with the det_Vvv info added
|
|
2422 ... like 2421 but with the det_VrtxtrackID negative if the signal consist of more than just one track
|
|
2421 ... like 2178 but with some new variables of det_??? added
|
|
|
|
2417 ... like 2181 but with 0.5 deg tilt in y
|
|
2416 ... like 2181 but with Al sample holder 4mm thick (instead of 2mm)
|
|
|
|
2301-2305 ... like 2201-2205 but for the simple tube geometry mimiking the old ALC.
|
|
2221-2226 ... like 2211-2216 but with the Cu cryostat added in the gap between the sample and rod.
|
|
2216 ... like 2211 but moved by 120 mm outside
|
|
2215 ... like 2211 but moved by 100 mm outside
|
|
2214 ... like 2211 but moved by 80 mm outside
|
|
2213 ... like 2211 but moved by 60 mm outside
|
|
2212 ... like 2211 but moved by 40 mm outside
|
|
2211 ... like 2202 but with the Cu rod added (simulates the holder of the cryostat)
|
|
2205 ... like 2201; Sample = 7mm Cu
|
|
2204 ... like 2201; Sample = 5mm Cu
|
|
2203 ... like 2201; Sample = 3mm Cu
|
|
2202 ... like 2201; Sample = 2mm Cu
|
|
2201 ... simple tube geometry mimiking the new ALC, Alexey wanted for the paper; Sample = 1mm Cu
|
|
|
|
|
|
2195-7 ... like 2181 but with the initial beam shifted by 2, 5 and 10 mm in y coordinate
|
|
2194 ... like 2181 but with oposite polarisation (100%)
|
|
2193 ... like 2181 but with polarisation = 100%
|
|
2192 ... like 2181 but with the 3mm sample and 1mm Pb shield
|
|
2191 ... like 2181 but with the 3mm sample
|
|
2190 ... like 2181 but with the 1mm Pb shield
|
|
2189 ... like 2181 but with the sample moved by 1mm forwards
|
|
2188 ... like 2181 but with the sample moved by 1mm backwards
|
|
2187 ... like 2181 but with the TURTLE beam
|
|
2186 ... like 2181 but with the point-like beam
|
|
2185 ... like 2181 but with homogeneous beam
|
|
2184 ... like 2181 but with momentum width 3MeV
|
|
2183 ... like 2181 but with p=26MeV
|
|
2182 ... like 2181 but with p=27MeV
|
|
2181 ... new default; like 2178 but with less variables stored
|
|
2178 ... new default: like 2113 but p=28MeV; Kapton; det_particleID added;
|
|
new field from Toni; polarisation =95%; all variables stored
|
|
2177 ... like 2113 but with the random polarisation after removing bug from 2176
|
|
2176 ... !! buggy !! like 2113 but with the random polarisation
|
|
2175 ... like 2113 but with the polarisation factor -100%
|
|
2174 ... like 2113 but with the oposit polarisation
|
|
2173 ... like 2113 but with the polarisation factor 0%
|
|
2172 ... like 2113 but with the polarisation factor 80%
|
|
2171 ... like 2113 but with the polarisation factor 95%
|
|
2162-8 ... like 2113 but with the muons generated just in front of the sample
|
|
at y = 0, 2.5, 5, 7.5, 10, 12.5 and 15 mm
|
|
2161 ... like 2113 but with the reuse of the calculated field values
|
|
2160 ... special file to calculate the mass of the ALC detector
|
|
2159 ... special file to study the effect of the kapton and Ti foils on the muon momentum
|
|
2158 ... like 2113 but with new ALC soleniod field map (calculated by Femlab (Tony)) with momentum of 26.00 MeV
|
|
2157 ... like 2113 but with new ALC soleniod field map (calculated by Femlab (Tony)) with momentum of 28.00 MeV
|
|
2156 ... like 2113 but with new ALC soleniod field map (calculated by Femlab (Tony)) with momentum of 29.79 MeV
|
|
2155 ... like 2113 but with quads (as found with Alexey) and parallel beam before quads.
|
|
2154 ... like 2113 but with TURTLE (by Kamil 90 cm before solenoid with momentum of 29.79MeV)
|
|
2153 ... like 2113 but with TURTLE (by Kamil 90 cm before solenoid)
|
|
2152 ... like 2113 but with TURTLE (by Robert 90 cm before solenoid)
|
|
2151 ... like 2113 but with the muon mean momentum of 28 MeV/c
|
|
2150 ... repete of 2113 (to test how long it runs)
|
|
2140-2146 like 2130-2136 but with oposite polarisation
|
|
2135 ... like 2130 but with cryostat of length=68mm.
|
|
2134 ... like 2130 but with cryostat of length=48mm.
|
|
2133 ... like 2130 but with cryostat of length=28mm.
|
|
2132 ... like 2130 but with cryostat of length=8mm.
|
|
2131 ... like 2130 but with cryostat of length=0mm.
|
|
2130 ... based on 2113 but sample holder removed (new ALC basic geometry to be compared with 2131-2135)
|
|
2128 ... like 2121 but with flat distributed beam in 20mm radius
|
|
2127 ... like 2121 but with just point-like beam
|
|
2126 ... like 2113 but with some more variables stored and with the beam offset and tilt that should compensate
|
|
2125 ... like 2113 but with some more variables stored and with the beam tilt
|
|
2124 ... like 2113 but with some more variables stored and with the beam offset
|
|
2123 ... like 2122 but with the oposite numbering of the scintillator detectors and reversed B field.
|
|
2122 ... like 2121 but with the oposite numbering of the scintillator detectors
|
|
2121 ... like 2116 but with some more variables stored
|
|
2111-2117 ... like 2101-2107 but with GEANT 4.9.1 and changes as in 2110
|
|
2110 ... like 2100 but with muon decay into two channels (also the radiative one)
|
|
2100 ... like 2051 but with GEANT 4.9.1
|
|
2101-2107 ... like 2091-2097, but after removing a small bug from ElementField
|
|
2097 ... new 3D field map ALC, globalfield, field in log_fieldvolume at 0.5, rotation 2 degree
|
|
2096 ... new 3D field map ALC, globalfield, field in log_fieldvolume at 0.5, rotation 1 degree
|
|
2095 ... new 3D field map ALC, globalfield, field in log_fieldvolume at 0.5, rotation 0.5 degree
|
|
2094 ... new 3D field map ALC, globalfield, field in log_fieldvolume at 0.5, rotation 0.25 degree
|
|
2093 ... new 3D field map ALC, globalfield, field in log_fieldvolume at 0.5
|
|
2092 ... new 3D field map ALC, globalfield, field in log_target at 0.5
|
|
2091 ... new 3D field map ALC, globalfield, field in log_target at 0.01
|
|
2090 ... test with the new 3D field map ALC
|
|
2084 ... like 2051 but with the signalSeparationTime = 200ns
|
|
2083 ... like 2051 but with the signalSeparationTime = 100ns
|
|
2082 ... like 2051 but with the signalSeparationTime = 25ns
|
|
2081 ... like 2051 but with the signalSeparationTime = 10ns
|
|
2078 ... like 2051 but muons generated just in front of the target at point at y=12
|
|
2076 ... like 2051 but muons generated just in front of the target at point at y=10
|
|
2075 ... like 2051 but muons generated just in front of the target at point at y=8
|
|
2074 ... like 2051 but muons generated just in front of the target at point at y=6
|
|
2073 ... like 2051 but muons generated just in front of the target at point at y=4
|
|
2072 ... like 2051 but muons generated just in front of the target at point at y=2
|
|
2071 ... like 2051 but muons generated just in front of the target at point at y=0
|
|
2070 ... like 2051 but muons generated just in front of the target (gaussian profile in x&y)
|
|
2065 ... Cryogenics, globalfield, field in log_fieldvolume at 0.5, rotation 2 degree
|
|
2064 ... Cryogenics, globalfield, field in log_fieldvolume at 0.5, rotation 1 degree
|
|
2063 ... Cryogenics, globalfield, field in log_fieldvolume at 0.5, rotation 0.5 degree
|
|
2062 ... Cryogenics, globalfield, field in log_fieldvolume at 0.5, rotation 0.25 degree
|
|
2061 ... Cryogenics, globalfield, field in log_fieldvolume at 0.5
|
|
2060 ... Cryogenics, globalfield, field in log_target at 0.5
|
|
2059 ... Cryogenics, globalfield, field in log_target at 0.01
|
|
2058 ... link to 2051
|
|
2057 ... repete of 2041 (just to be sure that I can reproduce the results of 2041)
|
|
2056 ... like 2021 but with the Cryogenics magnetic field
|
|
2055 ... like 2051 but with tilt in y of 0.5 degree
|
|
2054 ... like 2051 but with tilt in y of 0.25 degree
|
|
2053 ... like 2051 but with offset in y of 10 mm
|
|
2052 ... like 2051 but with offset in y of 5 mm
|
|
2051 ... like 2021 but with some unused variables commented out (to have smaller root output file)
|
|
2049 ... like 2021 but with the pitch 0.05
|
|
2048 ... like 2046 but with the pitch 0.05 (should slightly overfocuse focuse at 0T)
|
|
2047 ... like 2021 but with the tilt and offset (offset should add to the tilt at 0T)
|
|
2046 ... like 2021 but with the tilt and offset (offset should compensate the tilt at 0T)
|
|
2045 ... like 2021 but with the setlargestacceptablestep to 5 mm (instead of 200)
|
|
2044 ... like 2041 but with the setlargestacceptablestep to 5 mm (instead of 200)
|
|
2043 ... like 2041 but using the global field instead of magnetic field applied to log_World
|
|
2042 ... like 2041 but using the global field instead of magnetic field applied to log_target
|
|
2041 ... like 2021 but with the OI magnetic field
|
|
2034-6 ... like 2026 but with beam pitch
|
|
2031-3 ... like 2021 but with beam pitch
|
|
2029 ... like 2021 but with the turtle input (new turtle generated for high field)
|
|
2028 ... like 2027 but with the reversed initial polarisation
|
|
2027 ... like 2021 but with the muons generated just in front of the sample
|
|
2026 ... like 2021 but with the M counter
|
|
2025 ... like 2021 but with no sample (investigation of background)
|
|
2024 ... like 2023 + 1mm shield of Pb in the forward detector.
|
|
2023 ... like 2021 but with 3mm Cu Sample
|
|
2022 ... like 2021 + 1mm shield of Pb in the forward detector.
|
|
2021 ... 1mm Cu Sample; similar to 2003, but collimators at other position, modified sample holder
|
|
2015 ... like 2003 but with the 5mm sample
|
|
2014 ... like 2003 but with the far-away colimator off-axis by 10 mm
|
|
2013 ... like 2003 but with the near colimator off-axis by 10 mm
|
|
2012 ... like 2003 but with the beam tilt of 1.5 deg (no pitch)
|
|
2011 ... like 2003 but with the beam tilt of 0.5 deg (no pitch)
|
|
2008-10 ... different offsets of the magnetic field: 1cm in x, +/-3 cm in z
|
|
2007 ... like 2004 but with beam pitch and tilt
|
|
2006 ... like 2004 but with beam pitch and tilt
|
|
2005 ... like 2004 but with beam ofset by 10 mm.
|
|
2004 ... like 2002 but with thin tube detector holder (should correspond to alc_07_0523.dat)
|
|
2003 ... like 2002 but with large tube detector holder
|
|
2002 ... like 2001 but with larger target
|
|
2001 ... first test steering for the ALC test in December 2007 (the same steering as in 605.mac)
|
|
|
|
1400-1415 ... like 1371 but with large beampipe (larger than magnet allows, but the same as was in 1351)
|
|
1391 ... like 1371 (to have more statistics) ... 1371_1391 = 18*300000 events
|
|
1381 ... like 1371 but at B=0T
|
|
1371 ... like 1351 but with the split-coil Cryogenics field map (and narrower beampipe)
|
|
1361 ... like 1351 but at B=0T
|
|
1351 ... like 1339 but after some bugs removed; higher statistics;
|
|
1341 ... like 1338 but after some bugs removed
|
|
1339 ... like 1338 but with reweighting of events with muons in collimators
|
|
1338 ... active collimator with the segmented beam-pipe and with the TURTLE input file
|
|
1337 ... like 1336 but this time with event reweighting according to the collimator1 (reweighting by factor of 5)
|
|
1336 ... similer to 1335 but with broader beam and after modifying the simulation code to allow
|
|
us the event reweighting (however not used in this run)
|
|
1335 ... like 1332 but with the new version of the active collimator
|
|
1331-4 ... like 1321-4 but ???
|
|
1321-4 ... like 1311-4 but after migrating from magnetic to electromagnetic field in the F04GlobalField class
|
|
1314 ... based on 1313 but with the latest TURTLE input file
|
|
1313 ... based on 1312 but without the old "active collimator"
|
|
1312 ... like 1311 but with the G4Beamline-like magnetic field
|
|
1311 ... like 1174 (repete on 4 March 2008, after long time)
|
|
( old: 1200-13... like 1100-16 but with Cryogenics magnet instead of the OI. )
|
|
119? ... like 118? but with narrow beam
|
|
118? ... like 117? but with all events saved and Cu used in the active collimator instead of scintillator
|
|
117? ... With Coulomb scattering, Ti cryostat, active collimator and the following options
|
|
M0 counter M1 counter Cryostat Cu-wall
|
|
1172 200 mu - -
|
|
1173 200 mu - yes
|
|
1174 400 mu - yes
|
|
1175 200 mu 200 mu yes
|
|
1176 400 mu 400 mu yes
|
|
116? ... like 114? but after removing the bug
|
|
115? ... without Coulomb scatt. to compare with 114?
|
|
114? ... with Coulomb scattering (but buggy)
|
|
1131-4 ... like 1100 but with different l (1131 without M0 counter)
|
|
1120-21... just for testing with fine field map inside the sample.
|
|
1100-16... like 1050-1059 but with geant version 4.9.0 and larger target, sample and wider beam
|
|
1050-9...like 1035, but with 2000000 of events and different decaytimelimits
|
|
1029 ... l=20mm; d=20mm; scint= 3.63x3.63x3.63; decaytimelimits = 400-420ns, wide beam
|
|
1028 ... l=20mm; d=15mm; scint= 2.9x2.9x2.9; decaytimelimits = 400-420ns, wide beam
|
|
1025 ... l=20mm; d=12.2mm; scint= 2.5x2.5x2.5; decaytimelimits = 400-420ns, wide beam
|
|
1022 ... l=20mm; d=12.2mm; scint= 2.5x2.5x2.5; decaytimelimits = 10400-10420ns, wide beam
|
|
1021 ... l=20mm; d=12.2mm; scint= 2.5x2.5x2.5; decaytimelimits = 100400-100420ns, wide beam
|
|
1003-9 ... like 183-9 but with decaytimelimits = 10400-10420ns
|
|
1002 ... l=5mm; d=12.2mm,decaytimelimits = 100400-100420ns, wide beam
|
|
1001 ... l=5mm; d=12.2mm,decaytimelimits = 10400-10420ns, wide beam
|
|
1000 ... like 1002 but with the homogenious beam (not the Gaussian one)
|
|
193-9 ... like 183-9 but with focused beam
|
|
183-9 ... like 173-9 but with SetLargestAcceptableStep=4 and decaytime between 400 and 420 ns
|
|
179 ... like 173, with: l=20mm; d=20mm; scint= 3.63x3.63x3.63
|
|
178 ... like 173, with: l=20mm; d=15mm; scint= 2.9x2.9x2.9
|
|
177 ... like 173, with: l=20mm; d=20mm; scint= 2.5x2.5x2.5
|
|
176 ... like 173, with: l=20mm; d=15mm; scint= 2.5x2.5x2.5
|
|
175 ... like 173, with: l=20mm; d=12.2mm
|
|
174 ... like 173, with: l=10mm; d=12.2mm
|
|
173 ... New simple HiFi geometry suggested on the meeting on 13th June (Alex, Robert, Dirk)
|
|
l=5mm (distance from centre to cryostat backward wall);
|
|
d=12.2mm (inner distance of opposite scintilators)
|
|
172 ... like 170 but with old 3D field map.
|
|
171 ... like 170 but all events stored
|
|
170 ... like 165 but after changing the way how initial polarisation is defined.
|
|
168,9 ... like 165,6 but with old 3D field map.
|
|
167 ... like 166 but smaller beam momentum smearing.
|
|
166 ... like 165 but at 10 T
|
|
165 ... like 156 but with O.I. field map (now field map is read in in polar coordinates)
|
|
161 ... like 156 but no magnetic field
|
|
160 ... like 156 but no beam momentum and generated position smearing
|
|
159 ... like 156 but no beam momentum smearing
|
|
158 ... like 156 but without cryostat
|
|
156,157 ... like 154 and 155 but with GEANT 4.8.3; corrected titanium windows in the cryostat; SetLargestAcceptableStep=20;
|
|
155 ... like 154 but with decaytime between 1400 and 1440 ns
|
|
154 ... tubsbox; otherwise like 152
|
|
153 ... like 141 but with time info of the hits (signalSeparationTime=1ns)
|
|
152 ... like 141 but with time info of the hits (signalSeparationTime=0.1ns)
|
|
146 ... like 142 but now using G4CoulombScattering for muons
|
|
145 ... like 144 but with restricted beam width (sigma=2.5mm)
|
|
144 ... like 143 but without the magnetic field
|
|
143 ... like 142 but without the cryostats
|
|
142 ... like 141 but without beam smearing
|
|
141 ... HiFi with tubs; now with smaller range cut and beam size restricted to the beam
|
|
136 ... HiFi; TF=3T; (now with smaller range cut (was 1cm before, now 0.1mm and in target 0.01mm)
|
|
|
|
701 ... like 314 (i.e. the test ALC geometry to our best knowledge) for the updated code/steering.
|
|
(to reproduce 314, sign of the polarisation had to be changed from 1 to -1) (planned for October 2007 seminar).
|
|
615-8 ... reversally polarised muons to 605-8
|
|
605-8 ... like 602-4 but with all events (not only those with hits) (and plus 1.5 mm thickness) ;
|
|
602-4 ... new ALC with Cu sample of 1, 2 and 3 mm.
|
|
601 ... new ALC design with many details (test run)
|
|
561-6 ... like 543,544 but with changing the radius of the iron inner tube for the backward detector (not the forward!)
|
|
(R_Fe_back=30,40,45 mm) (+34mm for the runs 543,544).
|
|
551-8 ... like 543,544 but with changing the thickness of the iron inner tube for the backward detector (not the forward!)
|
|
(Fe_back_thickness=1,3,4,5 mm) (+2mm for the runs 543,544).
|
|
541-6 ... like 525&526 with the correct (inner) R_det=47 & 56 mm & different iron inner tubes of wall
|
|
thickness of 1,2 and 3 mm.
|
|
BUG IN SOME PREVIOUS RUNS: R_det was in fact not the inner radius but the radius in the middle of the scint.
|
|
531-538 ... like 521-530 but with l_target=3mm and l_det_backward=80,100,140,160mm (+runs 525&526 for 120mm).
|
|
521-530 ... segmented det; l_sep=2*2mm; l_det=120mm; Cu target; l_target= 1,2,3,4,5mm;
|
|
R_forw=47 mm; R_back=56 mm; different scintilator widths; added Fe tube 2mm;
|
|
511-520 ... like 501-510 but with the segmented detectors
|
|
501-510 ... l_sep=2*2mm; l_det=120mm; Cu target; l_target= 1,2,3,4,5mm; R_forw=42 mm; R_back=51 mm; added Fe tube 2mm;
|
|
491-500 ... l_sep=0; l_det=120mm; Cu target; l_target= 1,2,3,4,5mm; R_forw=45 mm; R_back=54 mm; added Fe tube 2mm;
|
|
481-484 ... like 445-6 but with added steel (2mm) or aluminium (4mm) tube
|
|
471-478 ... l_sep=0; l_det=150, 120, 100, 70 mm; Cu target; l_target= 3mm; R_det=47.5 mm + runs 449-450, 445-446
|
|
461-464 ... l_sep=0; l_det=200mm; Cu target; l_target= 3mm; R_back= 47.5 mm; R_forw=42.5, 37.5 mm
|
|
451-458 ... l_sep=0; l_det=200mm; Cu target; l_target= 3mm; R_forw= 47.5 mm; R_back=52.5, 57.5, 62.5, 67.5 mm
|
|
449-450 ... l_sep=0; l_det=170mm; Cu target; l_target= 3mm; R_det=47.5 mm
|
|
441-446 ... l_sep=0; l_det=200mm; Cu target; l_target= 3mm; R_det=27.5, 37.5 & 47.5 mm
|
|
431-436 ... l_sep=2*20mm; R_det=27.5mm; l_det=50, 100, 150 mm; Cu target; l_target= 3mm; (+ RUN 425 & 426 for l_det=200mm)
|
|
421-428 ... l_sep=2*20mm; R_det=27.5mm; l_det=200mm; Cu target; l_target=0.5, 1, 3, 5 mm;
|
|
409-14 ... like 389 and 408 but with the separation of 2*10, 2*20 and 2*30mm.
|
|
408 ... like 389 but with reversed polarisation
|
|
405-6 ... like previous but with the separation of 2*30mm
|
|
403-4 ... like previous but with the separation of 2*20mm
|
|
401-2 ... like 382 and 393 but with the separation between detectors of 2*10mm
|
|
393 ... like 382 but with reversed polarisation (0,0,1) instead of (0,0,-1)
|
|
389-392 ... like 382,386-8 with adding 3mm Cu after the target
|
|
386-8 ... like 382 but with increasing R_of_the_backward_detector=27.5, 30, 32.5 and 35
|
|
381-5 ... like 375-9 but NO COLLIMATOR !
|
|
376-9 ... like 375, but with R_beam_max = 20, 22.5, 25 and 27mm;
|
|
375 ... sigma_beam=11mm; R_beam_max=15mm; collimators on
|
|
370-1 ... like 364-5 but with the point-like shifted by 27 mm on the x axis
|
|
368-9 ... like 364-5 but with the point-like shifted by 18 mm on the x axis
|
|
366-7 ... like 364-5 but with the point-like shifted by 9 mm on the x axis
|
|
364-5 ... big target, but just a point-like beam
|
|
362-3 ... like 358-9 but with beam limited to just r=14mm (like in 354-7)
|
|
360-1 ... like 358-9 but with only water target without brass
|
|
358-9 ... like 356-7 but with wider target and beam
|
|
354-7 ... like 350-3, but with 11mm sigma of the beam width
|
|
350-3 ... like 346-9, but with 5mm sigma of the beam width
|
|
348-9 ... like 346-7, but with 200mm long detectors
|
|
346-7 ... water target, 100mm long detectors, point-like beam;
|
|
344-5 ... like 332-3 but after the implementation of 2D field possibility (just to check all remains OK)
|
|
342-3 ... like 332-3 but with 2mm target with centre at 0mm
|
|
340-1 ... like 332-3 but with 2mm target with centre at 1mm
|
|
338-9 ... like 332-3 but with beam of spacial spread of generated muons with sigma = 11mm
|
|
330-7 ... like 322-9 but with corrected detector diameter to 55mm, no separation gap, point-like beam
|
|
and thinner Cu target.
|
|
322-9 ... Simple ALC-like design (just tubes) with the length of scintilators = 50, 100, 200 and 300 mm
|
|
(study for Alexey and Robert).
|
|
320-1 ... like 314-315 but with the target shifted by 10 mm towards the back detector
|
|
318-9 ... like 314-315 but with the forward detector shifted by 5 mm in x direction
|
|
314-7 ... like 310-3 but with time info of the hits
|
|
310-3 ... (NEW DEFINITION!!!) like 290-4 but with 2mm PVC added behind the target.
|
|
312-3 ... (REWRITTEN!!!) like 292-3 but with target thickness of 1 mm instead of 0.8
|
|
310-1 ... (REWRITTEN!!!) like 290-1 but with Geant 4.8.3 - no change observed
|
|
304-9 ... like 290-1 but with G4CoulombScattering and just for 5 B-field values and 10000 events/fieldValue
|
|
300-3 ... like 290-3 but with G4CoulombScattering instead of G4MultipleScattering
|
|
292-3 ... Al target
|
|
290-1 ... like 260-1 but with solid aluminium tube in forward region added
|
|
278-83... like 268-73 but without target
|
|
274-5 ... repeated 260-1
|
|
272-3 ... like 268-9 but with beam tilt of 0.2 and 0.5 degree
|
|
270-1 ... like 268-9 but with vertex shifted by 4 and 9 mm
|
|
268-9 ... like 260-1 but with TURTLE BEAM PROFILE
|
|
262-7 ... different runs (all?) without target
|
|
260-1 ... NEW DEFAULT like 234-5 but with much smaller range cut (was 1cm before, now 0.1mm and in target 0.01mm)
|
|
254-5 ... like 234-5 but with penelope processes
|
|
252-3 ... like 234-5 but with lowenergy processes
|
|
250-1 ... like 234-5 but with forward dectector shifted by 10 mm
|
|
240-1 ... like 234-5 but with very simplified geometry
|
|
238-9 ... like 234-5 but with random tilt with sigma of 0.5 degree
|
|
236-7 ... like 234-5 but with tilt in y of 0.5 degree
|
|
234-5 ... ALC; target = 2mm Cu; changed beam properties
|
|
232-3 ... like 222-3 but with the beamwidth of 1mm
|
|
230-1 ... like 222-3 but with the momentum smearing of 10%
|
|
228-9 ... like 222-3 but with target shifted by 2mm in the forward direction
|
|
226-7 ... like 222-3 but without target
|
|
224-5 ... like 222-3 but with Cu 2mm target;
|
|
222-3 ... ALC; target = 0.8mm Al; detailed geometry description
|
|
220, 221 like 210&211 but muon source shifted to ~-1m
|
|
218, 219 like 210&211 but without target
|
|
216, 217 like 210&211 but with target shifted by 2mm in forward direction
|
|
214, 215 like 210&211 but with Cu 2mm target
|
|
212, 213 like 210&211 but with 1mm beam width
|
|
211 ... ALC; target = Al; B=2.3-5T; only three modules
|
|
210 ... ALC; target = Al; B=0-2T; only three modules
|
|
208 ... like 205 but with target = Al
|
|
207 ... like 204 but with target = Al
|
|
206 ... like 204 but with almost no beam width
|
|
205 ... ALC; target=Cu; B=2.3-5T
|
|
204 ... ALC; target=Cu; B=0-2T
|
|
201 ... ALC; design
|
|
|
|
116 ... like 110 but with the tube target (was box overlaping with detector region in 110)
|
|
115 ... 100k like 116 but with TF=3 Tesla;
|
|
114 ... 1M; tubsbox; TF=3 Tesla , emu20.dat, step=100mm; P=29MeV; cryostat included 31.049206h, 30.420839h
|
|
113 ... 1M; tubsbox; TF=3000 Gauss, emu20.dat, step=100mm; P=29MeV; cryostat included 2.5324222h, 2.4793444h
|
|
112 ... 1M; tubsbox; TF=3000 Gauss, uniform, step=200mm; P=29MeV; cryostat included 65.873625h, 64.539083h
|
|
111 ... 1M; tubsbox; TF=300 Gauss, uniform, step=200mm; P=29MeV; cryostat included; 0.97465h, 0.95433889h
|
|
110 ... 1M; small tube; TF=300 Gauss, uniform, step=200mm; P=29MeV; cryostat included; 1.1270083h, 1.0706889h
|
|
106 ... like 102 but putting in many more volumes
|
|
105 ... 1M; small tube; TF=3 Tesla from emu20.dat; P=29MeV;
|
|
104 ... 1M; small tube; TF=3000 Gauss from emu20.dat; P=29MeV;
|
|
103 ... 1M; small tube; TF=3000 Gauss; step=200mm; P=29MeV;
|
|
102 ... 1M; small tube; TF=300 Gauss; step=200mm; P=29MeV;
|
|
|
|
1 ... Transverse field 30 Gauss; strange ratio of Forward/Backward - why
|
|
not 1?
|
|
2 ... Like 1 but two more variable added to the Root Tree.
|
|
3 ... Transverse field 10e-6 T.
|
|
16... 1M; No field;
|
|
17... 1M; TF=30 Gauss
|
|
18... 1M; TF=300 Gauss
|
|
19... 1M; TF=30 Gauss; Delta_P/P = 0.05;
|
|
20... 1M; LF=30 Gauss; Delta_P/P = 0.
|
|
21... 1M; LF=30 Gauss; P=1MeV and Delta_P/P=0.3
|
|
22... 1M; TF=30 Gauss; P=1MeV and Delta_P/P=0.3
|
|
23... like 17 (to retest version 17, because 22 seems to be buggy)
|
|
24... 0.1M; TF=30 Gauss; P=3MeV and Delta_P/P=0.05
|
|
25... 1M; TF=300 Gauss; P=3MeV and Delta_P/P=0.05
|
|
26... debugging
|
|
27... 1M; TF=300 Gauss; P=29MeV; Gaussian magnetic field with B_RMS=5mm
|
|
33... 0.1M; TF=300 Gaus; P=29MeV; Delta_P/P=0.5 (with down limit)
|
|
34... like 33 but changed way of reading the posIniMomX Y Z in the program
|
|
36... 1M; TF=30 Gauss; P=29MeV; finer range cut = 1mm (was 1cm before)
|
|
37... 1M; TF=300 Gauss; P=29MeV;
|
|
38... 1M; TF=300 Gauss; Gaussian field (sigma=10mm)
|
|
39... 1M; TF=300 Gauss; Gaussian field; P=29MeV; momentum smearing
|
|
40... 10M; like 37
|
|
41... like 37 but with LF
|
|
42... like 38 but gaussian sigma = 5mm
|
|
43... like 38 but gaussian sigma = 8mm
|
|
44... 1M; P=29MeV; zero field
|
|
45... 1M; TF=300 Gauss; P=29MeV
|
|
46... 1M; TF=300 Gauss; P=29MeV; momentum smearing
|
|
48... 1M; TF=300 Gauss; P=3MeV; momentum smearing with sigma=1.5MeV, cutted
|
|
49... 100k like 45, however with new version of musr with the Geant4 muon decay with spin
|
|
51,53,54,55,58 ... like 4? but with the new version of musr with the Geant4 muon decay
|
|
70... 1M; TF=300 Gauss; P=29MeV
|
|
71... 1M; TF=300 Gauss; P=29MeV; tube geometry
|
|
72... 1M; TF=3000 Gauss; P=29MeV; delta P=0.05; tube geom;
|
|
73... 1M; TF=3000 Gauss; P=29MeV; delta P=0.5; tube geom;
|
|
74... like 71 but with separation gap of 10degrees between the scintilators.
|
|
75... 5M; like 73
|
|
76... 5M; like 72, random seed initialisation = 2
|
|
77... 1M; TF=0; P=29MeV; tube geom; random seed init=2
|
|
78... like 71 but with GEANT 4.8.2.p01 (and random seed initialsation =2)
|
|
79... like 78 but with the removed classes "musrParticleGun.cc" and "musrParticleGunMessenger.cc"
|
|
(was maybe using old geant version ?)
|
|
80... 100k; TF=300 Gauss; P=29MeV; tube geometry; GEANT 4.8.2.p01; random seed initialisation = 2
|
|
81... 100k; TF=300 Gauss; P=29MeV; tube geometry; GEANT 4.8.2.p01; random seed initialisation not set
|
|
82... like 80 but after change of the way how the random seed initialisation is done.
|
|
83... 10k; TF=3000 Gauss; P=29MeV; delta P=0.5; tube geom; GEANT 4.8.2.p01
|
|
84... like 80 but with another change how the random seed is initialised
|
|
85... 1M; TF=300 Gauss; P=29MeV; tube geometry; GEANT 4.8.2.p01; randomOption = 2 (back to code of 82)
|
|
87... like 71 but with the new way how the geometry is read in; GEANT 4.8.2.p01
|
|
88... test
|
|
90... like 71 but with the geometry read in from the steering file
|
|
91... like 90 but using "mm" instead of "cm" for the detector design (was wrong previously!!!)
|
|
- wrong thickness!!! Was 0.5mm, should be 5mm
|
|
92... correceted 91 (thickness of the scintilator 5mm)
|
|
98... like 71 but after merging the geometry_XX.txt file with the run_XX.mac file
|
|
99... like 92 ----------------------||-------------------------------------------
|
|
100... like 99 but with the magnetic field read in from the field map
|
|
|
|
|
|
130001 ... like 102202 (repetition)
|
|
|
|
120072 ... like 120062 but without G4MultipleScattering, G4MuBremsstrahlung and G4MuPairProduction
|
|
12006? ... like 12004? but without SetUserLimits log_??? 0.01
|
|
12005[2-4] ... (1.10.2009) like 12004[2-4] but without /musr/ignore SetUserLimits log_plate 0.01
|
|
120049 ... (1.10.2009) like 120014 but with SetUserLimits log_??? 0.01
|
|
12004[2-4] ... (30.9.2009) like 12003[2-4] but with momentum spread of the initial muons
|
|
120038 ... like 120032 but without SetUserLimits log_??? 0.01
|
|
12003[2-4] ... like 12002[2-4] but with no initial momentum spred of the muons and with
|
|
/musr/ignore SetUserLimits log_plate 0.01, and with start of the Cu material at z=0mm.
|
|
120024 ... (24.9.2009) like 120022 but Cu sample divided into two pieces (the first is 0.04 mm thick)
|
|
120023 ... (24.9.2009) like 120022 but Cu sample divided into two pieces (the first is 0.02 mm thick)
|
|
120022 ... (24.9.2009) like 120016 but Cu sample a little bit thicker
|
|
120020 ... (18.9.2009) like 120016, but with kapton tape moved just in front of the Cu sample
|
|
120019 ... (18.9.2009) like 120018, but with Cu moved just in front of the Cu sample
|
|
120018 ... (18.9.2009) like 120016, but with Cu tape instaed of kapton
|
|
120017 ... (10.9.2009) like 120014, but no air and no kapton (i.e. only Cu sample plate)
|
|
120016 ... (10.9.2009) like 120014, but no air
|
|
120015 ... (10.9.2009) like 120014, but no kapton
|
|
120014 ... (10.9.2009) similar to previous, but with kapton tape and air (like in the real ALC experiment)
|
|
120010 ... (9.9.2009) test of the penetration depth in the ALC experiment (Cu sample plate) vs. SRIM
|
|
120000 ... test with the 76MeV muons stopping in GPD experiment (done for Rustem)
|
|
|
|
======================================================================================
|
|
10433? ... like 10432? but with 10% (?) momentum smearing of initial muons
|
|
10432? like 10431? but without the collimators
|
|
104315 ... like 104313 but with mu-
|
|
104311-4 ... experiment for David Taqqu with the preassure of 5, 20, 40, 60 mbar
|
|
10430? ... modified experiments for David Taqqu
|
|
10424? ... large stat, 500 V electric field (oposit to 10423?)
|
|
10423? ... large stat, 500 V electric field
|
|
104220 ... large statistics
|
|
104212 ... based on 104202 but with Geant4.9.5, larger stat. and an additional collimator
|
|
104211 ... based on 104201 but with Geant4.9.5, larger stat. and an additional collimator
|
|
104208 ... like 104202 but with Geant4.9.5
|
|
104207 ... like 104201 but with Geant4.9.5
|
|
|
|
104202 ... like 104201 but with muons generated at rest in the volume of interest - to be
|
|
used for the detector efficiency calculations.
|
|
104201 ... real geometry as obtained from Aldo on 13.12.2011
|
|
|
|
104061 | 15MeV/c| 61 mum |
|
|
104062 | 15MeV/c| 62 mum |
|
|
104063 | 15MeV/c| 63 mum |
|
|
104064 | 15MeV/c| 64 mum |
|
|
104065 | 15MeV/c| 65 mum |
|
|
104066 | 15MeV/c| 66 mum |
|
|
104067 | 15MeV/c| 67 mum |
|
|
|
|
104051 | 12MeV/c| 44 mum |
|
|
104052 | 12MeV/c| 45 mum |
|
|
104053 | 12MeV/c| 46 mum |
|
|
104054 | 12MeV/c| 47 mum |
|
|
104055 | 12MeV/c| 48 mum |
|
|
104056 | 12MeV/c| 49 mum |
|
|
|
|
104041 | 10MeV/c| 19 mum |
|
|
104042 | 10MeV/c| 20 mum |
|
|
104043 | 10MeV/c| 21 mum |
|
|
104044 | 10MeV/c| 22 mum |
|
|
|
|
104020 | No collim | 1M events
|
|
104021 | 70 mm brass | 1M events
|
|
104022 | 70 mm PVC | 1M events
|
|
104023 | 20 mm brass | 1M events
|
|
|
|
104001 Experiment of Aldo (piE1 in October-November 2011):
|
|
|
|
======================================================================================
|
|
BEAMLINE OSCILLATIONS for Aldo:
|
|
103000: for Aldo ; beampipe for ALDO
|
|
103001: ALC magnet ; #piE3 TURTLE p=27.5#pm0.52MeV/c; measured (?) ALC field map
|
|
103002: ALC magnet ; #piE3 TURTLE p=10.0#pm0.19MeV/c; measured (?) ALC field map
|
|
103003: ALC magnet ; parallel beam p=10.0#pm0.30MeV/c; measured (?) ALC field map
|
|
103004: ALC magnet ; parallel beam p=10.0#pm0.30MeV/c; calculated ALC field map
|
|
103005: ALC magnet ; #piE3 TURTLE p=10.0#pm0.19MeV/c shifted; measured (?) ALC field map
|
|
103006: ALC magnet ; ideal focused beam, p=10.0#pm0.30MeV/c; measured (?) ALC field map
|
|
103007: ALC magnet ; prallel beam, p=10.0#pm0.30MeV/c; 25#mum scint.; measured (?) ALC field map
|
|
103008: ALC magnet ; prallel beam, p=10.0#pm0.30MeV/c; 29#mum scint.; measured (?) ALC field map
|
|
|
|
|
|
|
|
======================================================================================
|
|
|
|
102303 ... like 102302 but with a newer Turtle file from Davide Reggiani
|
|
102302 ... like 102301 but with larger statistics
|
|
102301 ... (21.3.2012) based on 102202 but updated to the latest design.
|
|
----
|
|
102202 ... like 102002 but using FOR070_2008_10_17_XXII.DAT turtle input file.
|
|
102102 ... (2008.10.20.) similar to 102002 but using FOR070_2008_10_17_XXII.DAT and including
|
|
new method to calculate the field integral along the muon path.
|
|
1020?? ... beam envelope using TURTLE input file "FOR070_2008_09_29_XII.DAT"
|
|
... like FOR070_2008_09_29_II.DAT but with delta p/p ~ 3% instead of ~1.5%
|
|
1020?? ... beam envelope using TURTLE input file "FOR070_2008_09_29_XI.DAT"
|
|
... like FOR070_2008_09_29_I.DAT but with delta p/p ~ 3% instead of ~1.5%
|
|
102002 ... beam envelope using TURTLE input file "FOR070_2008_09_29_II.DAT"
|
|
... based on the initial Robert's turtle file, but focused
|
|
better to z=-20cm at zero field (to have a different
|
|
TURTLE file to see a possible influence of the Turtle files)
|
|
102001 ... beam envelope using TURTLE input file "FOR070_2008_09_29_I.DAT"
|
|
... very similar to the initial Robert's turtle file, but focused
|
|
better to z=0 at zero field
|
|
|
|
|
|
|
|
101061-2 ... like 101051-2 but for the 2m long beampipe (i.e. for the ALC design)
|
|
101053 ... like 101052 but with the better focuse to the centre of the solenoid
|
|
101052 ... like 101051 but 10 times more events
|
|
101051 ... like 101021 but with some more save volumes also before the quadrupole triplet
|
|
101033 ... like 101032 but with the r=15mm collimator at z=-10cm
|
|
101032 ... like 101031 but with the r=20mm collimator at z=-80cm
|
|
101031 ... real quads focused to -20cm, TURTLE 60
|
|
101023 ... like 101022 but with the r=15mm collimator at z=-10cm
|
|
101022 ... like 101021 but with the r=20mm collimator at z=-80cm
|
|
101021 ... real quads focused to +10cm, TURTLE 60
|
|
101019 ... like 101013 but with the restricted beam radius at the quadrupoles (should be directly comparable to 101014)
|
|
101018 ... real quads (as found out with Alexey) with field gradients adujsted to focuse parallel beam to the centre
|
|
101014 ... Turtle61
|
|
101013 ... quadrupoles as in the TURTLE input file from Robert, the TURTLE output generated before the triplet (Turtle60)
|
|
101012 ... like 101011 but with the TURTLE beam before the quadrupole
|
|
101011 ... ALC with parallel beam before the quadrupoles, quadrupoles as measured with Alexey
|
|
101002 ... like 100392, but with the global field (implemented from F04 example from Gumplinger)
|
|
100411-24 ... like 100311-24 but for Cryogenics
|
|
100392 ... only "save" volumes, new TURTLE from Robert as is
|
|
100391 ... like 100387 but with less steps in the magnetic field
|
|
100390 ... only "save" volumes, gaussian parallel beam, tilt of the beam in y (corresponds to 5mm in the zero field)
|
|
100389 ... only "save" volumes, gaussian parallel beam, offset of the beam in y (5mm)
|
|
100388 ... only "save" volumes, gaussian parallel beam, smaller sigma in y than in x
|
|
100387 ... only "save" volumes, gaussian parallel beam
|
|
100386 ... only "save" volumes, focused beam
|
|
100385 ... only "save" volumes, TURTLE focused more or less to the centre.
|
|
100384 ... only "save" volumes, TURTLE as is
|
|
100381-3 ... using the new possibility of the "save" volumes
|
|
100331
|
|
100321-9 ... like 100311-4 but with small radius of M0 counter and of the Sample
|
|
100319 ... OI magnet; FWHM(p)=3%; pitch such that beam focused 10cm after the sample at 0 field
|
|
100318 ... OI magnet; FWHM(p)=3%; pitch such that beam focused 50cm after the sample at 0 field
|
|
100317 ... OI magnet; FWHM(p)=3%; TURTLE input file; pitch
|
|
100316 ... OI magnet; FWHM(p)=3%; TURTLE input file; no pitch
|
|
100315 ... OI magnet; FWHM(p)=3%; pitch such that beam focused 20cm before the sample at 0 field
|
|
100314 ... OI magnet; FWHM(p)=3%; pitch such that beam focused 5cm before the sample at 0 field
|
|
100313 ... OI magnet; FWHM(p)=3%; pitch such that beam focused to the sample at 0 field
|
|
100312 ... OI magnet; FWHM(p)=8%; no pitch
|
|
100311 ... OI magnet; FWHM(p)=3%; no pitch
|
|
100301 ... like 100161 but with the beam focused at 0 Field to the centre of the sample, i.e. to (0,0,0).
|
|
100221-4 ... like 100121-4 but with momentum spread FWHM=8%
|
|
100171-4 ... M0 counter = 0.4 mm , momentum spread FWHM=3%; R=5, 10, 15 & 20 mm; l=20mm with Cryogenics magnet
|
|
100161 ... M0 counter = 0.4 mm , momentum spread FWHM=3%; Gaussian beam; l=20mm,
|
|
100151-4 ... M0 counter = 0.4 mm , momentum spread FWHM=3%; R=5, 10, 15 & 20 mm; l=5mm
|
|
100141-4 ... M0 counter = 0.4 mm , momentum spread FWHM=3%; R=5, 10, 15 & 20 mm; l=20mm
|
|
100131-4 ... M0 counter = 0.4 mm , no momentum spread, R=5, 10, 15 & 20 mm; l=20mm
|
|
100121-4 ... no M0 counter, momentum spread FWHM=3%; R=5, 10, 15 & 20 mm; l=20mm
|
|
100111-4 ... no M0 counter, no momentum spread, R=5, 10, 15 & 20 mm; l=20mm
|
|
100101-2 ... 0.4 mm M0 counter, momentum spread, R=10&20mm; l=20mm
|
|
100002 ... like 100001 but muons start at -50cm.
|
|
100001 ... muon beam properties in the target: OI magnet, muons start at z =~ -130cm.
|
|
|
|
-------------------------------------------------------------------------------------
|
|
24632? ... like 24628 but with 100% diffusion scattering.
|
|
24631? ... like 24630? but air properties commented out - 10 times higher number of photons!
|
|
24630? ... to investigate why 24628? failed (World replaced by "vzduch") - no difference found
|
|
24629? ... like 24624? but with "polished unified" and diffusive scat. near edges.
|
|
24628? ... like 24621? but with 10% diffusive scat.
|
|
24627? ... like 24622? but 5x5 mm.
|
|
24626? ... like 24621? but 5x5 mm.
|
|
24625? ... like 24620? but 5x5 mm.
|
|
24624? ... like 24620? but with the "groundair LUT" near edges (0.1 mm)
|
|
24623? ... like 24620? but with the bevelled edges
|
|
24622? ... like 24620? but with "polishedair LUT" surface
|
|
24621? ... like 24620? but with "polished unified" surface
|
|
24620? ... B418, SPTR=230, ideal box, ideal surface (20.7.2012)
|
|
|
|
24615? ... like 24604? but with polishedteflonair LUT
|
|
24614? ... like 24604? but with the beam off-center (Alexey wanted to see if it plays a role)
|
|
24613? ... like 24605 but for thinner scintillator bar
|
|
24610-2? ... like 24607?-9? but for the scintillator BC418
|
|
24607-9? ... like 24604?-6? but for attenuation length of 80 mm
|
|
24606? ... like 24603?, SPTR=230; tau1=0.35; tau2=1.6
|
|
24605? ... like 24603?, SPTR=120; tau1=0.35; tau2=1.6
|
|
24604? ... like 24603?, SPTR= 0; tau1=0.35; tau2=1.6
|
|
24603? ... study on the long scintillator bar: SPTR=0; tau1=0; tau2=0
|
|
|
|
2455?? ... like 2448?? but with 60x40 APD cells
|
|
2454?? ... like 2448?? but with just 1 APD cell
|
|
2453?? ... like 2448?? but with 6x4 APD cells
|
|
2452?? ... like 2447?? but with just 1 APD cell
|
|
2451?? ... like 2447?? but with 6x4 APD cells
|
|
2450?? ... like 2443?? but with even small detector (1000 x smaller than normal size).
|
|
2448?? ... like 2424?? but with 100% reflectivity
|
|
2447?? ... like 2437?? but with 100% reflectivity
|
|
2446?? ... like 2436?? but with 100% reflectivity
|
|
2445?? ... like 2435?? but with 100% reflectivity
|
|
2444?? ... like 2434?? but with 100% reflectivity
|
|
2443?? ... like 2442?? but with extremely small detector
|
|
2442?? ... like 2434?? but with rise times of 0
|
|
2441?? ... based on 2434?? for rise times of 0, 0.063, 0.35, 1.0
|
|
and decay times of 1, 1.32, 1.6, 5., 15 and 43.8
|
|
2440?? ... like 2422 but with the random time jitter of 120 ps
|
|
243941 ... like 243841 but for LaBr3
|
|
243841 ... like 243810 but with the RESOLUTIONSCALE=2.5 (to have amplitude smearing
|
|
for the comparison with Seifert)
|
|
243[8-9] ... like 2427?? and 2428?? but random time jitter of 120 ps
|
|
243[4-7] ... like 2420 2423 2424 2425 but random time jitter of 120 ps
|
|
243[0-3] ... like 2420 2423 2424 2425 but with rise/decay times of 0.063 and 1.32
|
|
2428?? ... like 2424??, but for LaBr3 scintillator (Seifert)
|
|
2427?? ... like 2424??, but for LYSO scintillator (Seifert)
|
|
2426?? ... like 2422 but with the shorter rise and decay times
|
|
2425?? ... 2424?? + 2400 APD cells
|
|
2424?? ... 2423?? + random time jitter of 230 ps (i.e. should replace previous 224950)
|
|
2423?? ... 2420?? + cross talk of 0.11 (i.e. should replace previous 224900)
|
|
2422?? ... based on 2218?? - i.e. experimental setup modified according to 2420??, higher light yield
|
|
2421?? ... based on 2218?? - i.e. experimental setup modified according to 2420??
|
|
2420?? ... based on 2248?? but with GEANT 4.9.5 (10.1.2012) run on Merlin4,
|
|
rise/decay times of 0.35 and 1.6 respectively, and CFD delay of 1.5 ns.
|
|
-------------------------------------------------------------------------------------
|
|
230001-5 ... test for Alexey: muons passing through scintillator of different thicknesses
|
|
-------------------------------------------------------------------------------------
|
|
|
|
2256?? ... like 2248?? but run on Merlin4 (9.1.2012)
|
|
2251??- ... like 2249?? + finite nr. of cells effect (60x60 cells)
|
|
225001- ... like 224801 + finite nr. of cells effect (6x6 cells)
|
|
224901- ... like 224801 + cross talk
|
|
224801- ... repetition of 223301 after modifications of the code
|
|
--------- end of October 2011: Changes in the programm (cross-talk added, cell jitter changed)
|
|
|
|
224201-62 ... like 2239?? but with the finite nr. of cells effect (1x1 cells)
|
|
224101-62 ... like 2239?? but with the finite nr. of cells effect (6x6 cells)
|
|
224001-62 ... like 2239?? but with the finite nr. of cells effect (60x60 cells)
|
|
223901-62 ... wide electron beam covering the full scintillator area
|
|
223301-862 ... like the previous runs, but after correcting the "dielectric_LUT" bug.
|
|
... statistics increased.
|
|
MISTAKE in the previous runs - surface of the scintillator was wrongly defined
|
|
("dielectric_dielectric" instead of "dielectric_LUT")
|
|
222801-62 ... like 222801-62 but with statistical fluctuations for photon creation
|
|
222701-62 ... like 222301-62 but with statistical fluctuations for ionis. losses
|
|
222601-62 ... like 222301-62 but rise time=0.35, decay time=1.32.
|
|
222501-62 ... like 222301-62 but rise time=0., decay time=1.32.
|
|
222401-62 ... like 222301-62 but rise time=0.35, decay time=1.6.
|
|
222351-62 ... like 222301-12 but sigma(APD)=100ps.
|
|
222301-12 ... light transport in a single counter; ionisation losses and photon creation
|
|
without statistical fluctuations.
|
|
Rise time=0.063, decay time=1.32, sigma(APD)=0ps.
|
|
|
|
222021-2
|
|
222001 ... simplified simulation of 221131, where there is just one counter, and
|
|
2 MeV electron is generated at its entrance.
|
|
|
|
-------------------------------------------------------------------------------------
|
|
|
|
221951-67 ... like 221921-37 but with a different APD responce function
|
|
(APDpulseShapeFile_2011_Fitted.txt)
|
|
221921-37 ... like 221801 but with CFD information
|
|
221801 ... 4.11.2011 - based on 225101 and 221701
|
|
221401 ....13.10.2011 - based on 223901 and 221131
|
|
|
|
221301 ... like 221131 but smaller statistic and without plastic holders
|
|
221211 ... like 221131 but smaller statistic and scint rise time = 1.0ns
|
|
221201 ... like 221131 but smaller statistic and scint rise time = 0.75ns
|
|
221191 ... like 221131 but smaller statistic and scint rise time = 0.5ns
|
|
221181 ... like 221131 but smaller statistic and scint rise time = 0.35ns
|
|
221171 ... like 221131 but smaller statistic and scint rise time = 0.2ns
|
|
221161 ... like 221131 but smaller statistic and scint rise time = 0.1ns
|
|
221151 ... like 221131 but smaller statistic and scint rise time = 0.03ns
|
|
221141 ... like 221131 but smaller statistic and scint rise time = 0.0ns
|
|
|
|
221134 ... like 221131 but using 0.1 ps of random time scattering (instead of 100ps)
|
|
221133 ... like 221131 but using APDpulseShapeFile_2011_1e_H.txt
|
|
221132 ... like 221131 but delay time back to 1.5 ns
|
|
221131 ... like 221101_8 but after implementing CFD array & delay time=0.5 ns
|
|
|
|
221123 ... like 221101-8 but using CFD delay of 0.8 ns
|
|
221122 ... like 221101-8 but using CFD delay of 0.7 ns
|
|
221121 ... like 221101-8 but using CFD delay of 0.6 ns
|
|
221120 ... like 221101-8 but using CFD delay of 0.4 ns
|
|
221119 ... like 221101-8 but using CFD delay of 0.3 ns
|
|
|
|
221118 ... like 221101-8 but using CFD delay of 4.0 ns
|
|
221117 ... like 221101-8 but using CFD delay of 3.0 ns
|
|
221116 ... like 221101-8 but using CFD delay of 2.0 ns
|
|
221115 ... like 221101-8 but using CFD delay of 1.0 ns
|
|
221114 ... like 221101-8 but using CFD delay of 0.5 ns
|
|
221113 ... like 221101-8 but using CFD delay of 0.2 ns
|
|
221112 ... like 221101-8 but using APDpulseShapeFile_2011_1e_H.txt (steeper pulse rise)
|
|
221111 ... like 221101-8 but using 0.1 ps of random time scattering (instead of 100ps)
|
|
221101-8 ... new big simulation using APDpulseShapeFile_2011_1e_Z.txt
|
|
221086 ... like 221084 but after a change of stacking order for optical photons.
|
|
221083,84 ... with a newer APD response function
|
|
221061-4 ... like 221051-4 but after changing the CFD signal shaping and introducing some other
|
|
... definitions of odet_timeC and odet_timeD.
|
|
221051-4 ... implementing also rise time of the photons in the scintillator, but there were some bugs.
|
|
221041-4 ... like 221032 but after correcting bug in mean time + different random option in some runs
|
|
221033 ... like 221032 but APD readout from both sides
|
|
221032 ... like 221031 but /musr/command OPSA CFD -0.2 1.5 -1.8
|
|
221031 ... like 221011 but /musr/command OPSA CFD -0.3 2. -1.8 + plastic holders, huge statistics
|
|
|
|
221014 ... like 221011 but /musr/command OPSA CFD -0.3 0.5 -1.8
|
|
221013 ... like 221011 but /musr/command OPSA CFD -0.1 2. -1.8
|
|
221012 ... like 221011 but /musr/command OPSA CFD -0.2 2. -1.8
|
|
221011 ... like 104 (i.e. Sr source, C1 and C2 positron counters) including optical photons
|
|
... /musr/command OPSA CFD -0.3 2. -1.8
|
|
221000 ... again some Sr Tests, after long time. Now with Geant 4.9.4. (Feb 2011).
|
|
|
|
220051-9 ... different fields
|
|
220001 ... muSR time asymmetry measurement in the ALC magent - test for Alexey
|
|
|
|
210013 ... TOF measurement of the G-APDs in the ALC magnet using C1 and C2 positron counters; electrons as beam; B=4.8T - Coulomb sc.
|
|
210012 ... TOF measurement of the G-APDs in the ALC magnet using C1 and C2 positron counters; electrons as beam; B=0T
|
|
210011 ... TOF measurement of the G-APDs in the ALC magnet using C1 and C2 positron counters; electrons as beam; B=4.8T
|
|
210002 ... TOF measurement of the G-APDs in the ALC magnet using C1 and C2 muon counters; muons as beam; B=0T
|
|
210001 ... TOF measurement of the G-APDs in the ALC magnet using C1 and C2 muon counters; muons as beam; B=4.8T
|
|
|
|
200037 ... Sr test with just C1 and C2 of the size 3x3x2mm
|
|
200031-35 ... Sr test with just C1 and C2 of the size 4x4.6x2 mm
|
|
200021 ... muons stopped in the centre of the sphere; C1=5mm, C3=20mm
|
|
200019 ... like 200013 but with only C1 and C2 (to test new idea of Alexey)
|
|
200018 ... Sr experiment with C1 and C2 moved very close to C3
|
|
200013-7... Sr experiment in the set-up as in the case of the Alexey's experiment (C1=2mm, C2=2mm, C3=60mm)
|
|
200011 ... Strontium source emiting beta electrons towards the sphere detectors (C1=2mm, C2=2mm, C3=20mm)
|
|
200008 ... like 200007, but with 5 MeV positrons as a source
|
|
200007 ... like 200004, but with 30 MeV positrons as a source
|
|
200006 ... Strontium source emiting beta electrons towards the sphere detectors (the first one is 0.2 mm thick + 0.3mm Cu)
|
|
200005 ... Strontium source emiting beta electrons towards the sphere detectors (the first one is 0.2 mm thick)
|
|
200004 ... Strontium source emiting beta electrons towards the sphere detectors (the first one is 5 mm thick)
|
|
200003 ... Strontium source emiting beta electrons towards the sphere detectors (the first one is 2 mm thick)
|
|
|
|
|
|
PICTURES:
|
|
|
|
HiFi_01.eps: - longitudinal cross-section through the HiFi detector.
|
|
visual.mac with
|
|
/vis/viewer/zoom 20
|
|
/vis/viewer/set/sectionPlane on 0 0 0 cm -1 0 0
|
|
and setting z coordinate to 15 (mm?)
|
|
|
|
|
|
Field Integral for OI for Robert (mean value =1.45 Tm):
|
|
root [1] TFile* f=new TFile("data/musr_102151.root")
|
|
root [2] t1->Draw("BzIntegral","(BzIntegral>-2)&&(muDecayDetID==1201)")
|
|
|