- 04 Mar, 2022 1 commit
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Eoin Clerkin authored
Placement of tof_v20c and tof_v21a placement is corrected. This commit overwrites existing geometries. Defines the local tof origin to be the most upstream postion which is the front surface of the frame.
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- 02 Mar, 2022 5 commits
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PSD parking postion is intended for the hadron and muon setups. Hadron setup files updated. PSD parking postion is 18m from target, shifted to left by 0.9 m and lowered by 0.7 m.
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- 25 Feb, 2022 2 commits
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The MVD for sis100_electron is changed to v20a. The MVD is removed from sis100_hadron_DEC21 setup. At FU request, it is also removed from sis100_hadron and sis100_hadron_APR21 setups.
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- 21 Feb, 2022 1 commit
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Administrator authored
This geometry files only adds copy numbers to the nodes. The geometry itself hasn't changed.
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- 18 Feb, 2022 1 commit
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Eoin Clerkin authored
Fixes magnet_v21b position. Update trd tag in DEC21 lmvm setup.
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- 15 Feb, 2022 3 commits
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David Emschermann authored
add mCBM 2022 06 setup consisting only of STS, TOF, RICH and PSD, ,as discussed in the SIM meeting of Feb 15th
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Administrator authored
The GDML file is a copy of rich_v17a_1e.gdml where the names of the rich volume is changed from rich_v17a_1e to rich_v21a. The ROOT geometry was created with macro/rich/Import_GDML_Export_ROOT.c as it is added with CbmRoot MR 714.
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- 10 Feb, 2022 2 commits
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Pierre-Alain Loizeau authored
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Pierre-Alain Loizeau authored
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- 09 Feb, 2022 1 commit
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David Emschermann authored
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- 04 Feb, 2022 2 commits
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David Emschermann authored
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- 03 Feb, 2022 1 commit
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Eoin Clerkin authored
See computing/cbmroot!684 for details 7.0 cm shift in the z displacement v22b with box v22c without box
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- 01 Feb, 2022 1 commit
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Eoin Clerkin authored
These are same as v22a and v22b but with corrected radiation as discussed in mCBM meeting 2022-02-01 The setup files were modified accordingly.
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- 27 Jan, 2022 3 commits
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Eoin Clerkin authored
Uses new MVD binaries and updates to use tof v21a
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Eoin Clerkin authored
One for vertexing and tracking modes. Shifts mvd_v20c geometries by 40 cm consistent with the change of coordinate system.
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- 26 Jan, 2022 1 commit
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David Emschermann authored
add mSTS v22a which implements its aluminium box and include it to the mcbm setup 2022_01, refs #2404
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- 24 Jan, 2022 1 commit
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Eoin Clerkin authored
Includes media.geo with BP material definiations. Corrects radiaiton length miscalculation in MR CbmSoft/cbmroot_geometry!119
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- 23 Jan, 2022 1 commit
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Eoin Clerkin authored
One each for the hadron, electron and muon setups.
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- 13 Jan, 2022 2 commits
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Since Pascal left CBM Alexandru and Philipp are assigned as code owners for the trd directory.
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Eoin Clerkin authored
Correct missing function names.
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- 23 Dec, 2021 3 commits
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Eoin Clerkin authored
Add pipe_v16e_1e Add much/much_v21c_sis100_1m_jpsi.geo.root add much/much_v21c_sis100_1m_jpsi.geo.root pipe_v16e is the same as pipe_v16b only shifted by 40cm much_v21c is shifted much_v21a geometries Removes tof_v21a as DEC21 default As still awaiting MR.
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Eoin Clerkin authored
v21c which are v21a shifted to new coordinate system Bug fixes in setup files. PSD to psd_v20c in hadron shifted field to origin for lmvm and jpsi default pipe changed to v16e_1e adds info files for subsystems
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Eoin Clerkin authored
Bug: sts_v20a was missing from repo. sts_v20a is the same as sts_v19a only that it is shifted by 40~cm downstream consistent with a change of the global coordinate system from old target position to the center of the magnet. Translation is not done via a seperate matrix included with the TFile, instead internal via a transaltion between the top and sts_v20a volumes.
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- 22 Dec, 2021 1 commit
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Eoin Clerkin authored
Electron, Hadron, JPSI and LMVM setups use new coordinate system, each dectector is written with reference to the centre of the magnet, instead of the old target position. Old setup_sis100_[electron,hadron,jpsi,hadron.C renamed to setup_sis100_[electron,hadron,jpsi,hadron]_APR21.C with the intenstion that they will be deleted in the near future. Candidate default geometries for the DEC21 SW release are available at setup_sis100_electron_DEC21.C and similarily for other setups. long_sts setup is removed from setup directory.
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- 19 Dec, 2021 1 commit
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Mehulkumar Shiroya authored
There are four sts beampipe can be used with different sts_version as described below v21a: Old beampipe, can only be used with sts geometry version: sts_v21[a]. v21b: New beampipe. It has 40mm diameter upstream side and 104mm diameter (including cylindrical part) downstream side. This beampipe can be used with the sts geometry version: sts_v21[b, d, f, h]. v21c: New beampipe. It has 55mm diameter upstream side and 104mm diameter(including cylindrical part) downstream side. This beampipe can be used with the sts geometry version: sts_v21[c]. v21d: New beampipe. It has 40mm diameter upstream side and 104 diameter(including cylindrical part) downstream side. This beampipe can be used with the sts geometry having a target position at -44 cm. which means it can only be used with the sts geometry vesrion: sts_v21[e, g, i].
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- 17 Dec, 2021 2 commits
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Eoin Clerkin authored
magnet_v21a is the shifted verison of v20a magnet_v21b is the shifted verison of v20b rich_v21a is the shifted verison of v17a_1e Shifted by 40cm consistent with the change of coordinates from old target position to centre of the magnet. Having seperate translation for pipe_v16c causes problems for inclusion of MVD. Translation via node shift instead.
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Eoin Clerkin authored
As created by their respecitive macros.
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- 24 Nov, 2021 1 commit
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Mehulkumar Shiroya authored
STS v21h: The geometry has the target positioned at -4 cm. It can be used with the beampipe 40mm diameter upstream side and 104mm diameter downstream side. It has a beampipe flange on the back-side of the STS wall. In addition, the geometry has a sensor thickness 320 um which is similar thickness of the real silicon sensors purchased from the Hamamatsu Photonics for the use in the real experiment. Furthermore,the mico-cable is defined as a single volume attached to the silicon sensors. Micro-cable thickness (320 um) is choosen and the material Manganese is taken based on the calculation done based on the current microcable design, thickness and its material. The material is defined as STS_Manganese in the media.geo file. STS v21i: The geometry has the target positioned at -44 cm from the center of the magnet. It can be used with the beampipe 40mm diameter upstream side and 104mm diameter downstream side. It doesn't have a beam-pipe flange on the back-side of the wall. In addition, the geometry has a sensor thickness 320 um which is similar thickness of the real silicon sensors purchased from the Hamamatsu > for the use in the real experiment. Furthermore,the mico-cable is defined as a single volume attached to the silicon sensors. Micro-cable thickness (320 um) is choosen and the material Manganese is taken based on the calculation done based on the current microcable design, thickness and its material. The material is defined as STS_Manganese in the media.geo file. updated binaries files and media.geo file with a material name STS_Cable_21
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- 19 Nov, 2021 2 commits
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Mehulkumar Shiroya authored
Transformation between local sts origin (last station) and global origin (center of magnet) is now 59.5. Front face of sts to intended position of target (-44cm) is now 1.6 cm.
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Mehulkumar Shiroya authored
v21f: STS geometry is similar to the version v21b. The target position considered from -4 cm. The geometry can be used with the beampipe with diameter 40 mm upstream side and 104 mm downstream side. The geometry has beampipe flange on the back-side of the wall. v21g: STS geometry is similar to the version v21e. The target position is at -44 cm considering global origin from the center of magnet. The STS local coordinate is from the last station. In both geometry, the STS box and the beam pipe flange is made of Carbon fiber: The material has 70% carbon fiber with density 1.75 g/cm3 and epoxy resin (30%) with density 1.2 g/cm3. The material is defined in media.geo file as STS_CarbonFiber_21.
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- 18 Nov, 2021 1 commit
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Alexandru Bercuci authored
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- 17 Nov, 2021 1 commit
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Alexandru Bercuci authored
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