Before the time was calculated for each raw message, now it is calculated once per µSlice.

Due to some missed casting to double values, the UTC time stored in the CbmTrdRawMessageSpadic lost precision.
Now we also only store the time relative to the Timeslice in the 2021+ unpacker, such that a double is large enough to store the full information.

Administrator authored 3 years ago and Florian Uhlig committed 3 years ago

Add functionality to check if the macro dif finish successful.
The decision can be done on base of the return value as well as on base of
a string printed at the end of the macro.
Don't check the return value yet since oOn some system there are errors when
destructing the root session. Use only the printout from the macro to decide
if the macro finished successful.

Administrator authored 3 years ago and Florian Uhlig committed 3 years ago

The script contained two problems. The first one was a typo in the shebang.
The second problem was in the grep command. If the full path includes by
chance the string "so" or "dylib" all files of the directory were found
accidentally. Requiring "so" or "dylib" to be at the end of the line fixes
the error.

Administrator authored 3 years ago and Florian Uhlig committed 3 years ago

Installl CbmRoot and remove part of the source directory

Add code which tests if the installtion of CbmRoot works and if the installed
version is functional. Test the "make install" target and run some macros from
teh installation directory.

To be able to test the CbmRoot installation it is necessary that no header
files are accessible in the source directory since this is the fallback for
ROOT when compiling a macro. To achieve this the directories containing any
headers are removed from the source directory.
This is a dangerous operation when executed in a source directory used for
active development. The installation test should only be used when running
the CI/CD workflow.

Mehulkumar Shiroya authored 3 years ago and Florian Uhlig committed 3 years ago

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 by taking the current microcable design, thickness and its material.

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 by taking the current microcable design, thickness and its material.

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 -40 cm considering global origin
from the center of magnet. The STS local coordinate is from the last station.
The geometry can be used with the beampipe with diameter 40 mm upstream side and 104 mm downstream side.

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.

Change in tranformation from global origin (centre of magnet) to local origin of sts (last station) to a 59.5cm shift.
Front face of sts from a target placed at 44cm is now 1.6 cm.

Volker Friese authored 3 years ago and Florian Uhlig committed 3 years ago

Integration of cbm::algo::EventBuilder in the FairRoot run/task framework, with the new task CbmTaskBuildEvents. Included into regular testing. Refs #2271.

Volker Friese authored 3 years ago and Pierre-Alain Loizeau committed 3 years ago

Enabled setting parameters for single STS ASICs. Expanded ASIC parameter container by time offset and coefficients for walk correction.

Dominik Smith authored 3 years ago and Florian Uhlig committed 3 years ago

CbmTrdHitProducerQa: Fetching TrdPoints and MC tracks from CbmMCDataManager instead of FairRootManager.

Dominik Smith authored 3 years ago and Florian Uhlig committed 3 years ago

- Histograms are now produced separately for residual and pull distributions.
- Enabled auto-extension of histogram axes.
- TrdPoint positions used are now mean of 'in' and 'out' values.
- Added residual and pull for hit times.
- Removed some root data types.

Dominik Smith authored 3 years ago and Florian Uhlig committed 3 years ago

CbmTrdHitProducerQa: Histograms are now produced for a pre-selected number of planes (set by user, default = 4). Added CbmQaCanvas containers for all histograms (layer-wise).