EIC issueshttps://eicweb.phy.anl.gov/groups/EIC/-/issues2021-09-23T15:58:10Zhttps://eicweb.phy.anl.gov/EIC/juggler/-/issues/14GEM strip digitization2021-09-23T15:58:10ZWhitney ArmstrongGEM strip digitizationAdd strip digitization for gem readout.Add strip digitization for gem readout.Whitney ArmstrongWhitney Armstrong2020-09-17https://eicweb.phy.anl.gov/EIC/detectors/solid/-/issues/1Clustering in calorimeter2021-09-23T15:48:36ZWhitney ArmstrongClustering in calorimeterCalorimeter clustering in solid calorimeters.Calorimeter clustering in solid calorimeters.Chao PengChao Peng2020-08-13https://eicweb.phy.anl.gov/EIC/NPDet/-/issues/56Update B0 Magnet2021-09-23T15:48:48ZWhitney ArmstrongUpdate B0 MagnetThe design of the B0 magnet changedThe design of the B0 magnet changedEIC beamline and IR integrationTom PolakovicTom Polakovic2020-07-29https://eicweb.phy.anl.gov/EIC/detectors/ip6/-/issues/11Merge in content from accelerator repo2021-09-23T15:34:19ZSylvester JoostenMerge in content from accelerator repohttps://eicweb.phy.anl.gov/EIC/detectors/ip6/-/issues/7Accelerator effects2021-09-23T15:29:25ZDmitry RomanovAccelerator effectsOne should be able to turn on certain accelerator effects related to crabing and bunch geometry. That includes vertex smearing, initial particle angular and momentum smearing.
Discussion. Those effects are not implemented for the commo...One should be able to turn on certain accelerator effects related to crabing and bunch geometry. That includes vertex smearing, initial particle angular and momentum smearing.
Discussion. Those effects are not implemented for the common MCEG and there is a question if those should be implemented in full simulation software or some intermediate software (which is used for MCEG formats conversion). Moreover, many generators don't even simulate crossing angle.https://eicweb.phy.anl.gov/EIC/benchmarks/detector_benchmarks/-/issues/33Asymmetry in hcal z position2021-09-23T15:27:09ZRobinpreet DhillonAsymmetry in hcal z positionWhen we plot the Hit Position in z vs. the difference between the Hit Position and the Truth position, there's an asymmetry that favors large Hit z. The density/color distribution is expected but the favoritism at large z is not. Possibl...When we plot the Hit Position in z vs. the difference between the Hit Position and the Truth position, there's an asymmetry that favors large Hit z. The density/color distribution is expected but the favoritism at large z is not. Possible bug, or is there an explanation?
![2dHistZ](/uploads/1f8e102f9509d4636186649cf6ef78f6/2dHistZ.png)https://eicweb.phy.anl.gov/EIC/benchmarks/performance_display/-/issues/1GraphQL API missing individual artifacts2021-09-23T15:25:22ZWhitney ArmstrongGraphQL API missing individual artifactsGo to https://eicweb.phy.anl.gov/-/graphql-explorer and try the following:
```
query {
project(fullPath:"EIC/benchmarks/detector_benchmarks"){
id
name
# first 10 means the most recent 10
pipelines(first:10) {
edg...Go to https://eicweb.phy.anl.gov/-/graphql-explorer and try the following:
```
query {
project(fullPath:"EIC/benchmarks/detector_benchmarks"){
id
name
# first 10 means the most recent 10
pipelines(first:10) {
edges {
node {
id
jobs {
edges {
node {
id
artifacts {
edges {
node {
downloadPath
fileType
}
}
}
}
}
}
}
}
}
}
}
```
See gitlab issue: https://gitlab.com/gitlab-org/gitlab/-/issues/330934https://eicweb.phy.anl.gov/EIC/benchmarks/detector_benchmarks/-/issues/30Fix ecal barrel to work with athena2021-09-23T15:26:25ZWhitney ArmstrongFix ecal barrel to work with athenaEcal barrel benchmarks do not work with athena. Maybe just copying over the ecal design will fix it?
Job [#95047](https://eicweb.phy.anl.gov/EIC/benchmarks/detector_benchmarks/-/jobs/95047) failed for 4801aa52ccd87b3728ebe393e010cc822ed...Ecal barrel benchmarks do not work with athena. Maybe just copying over the ecal design will fix it?
Job [#95047](https://eicweb.phy.anl.gov/EIC/benchmarks/detector_benchmarks/-/jobs/95047) failed for 4801aa52ccd87b3728ebe393e010cc822edabbbc:https://eicweb.phy.anl.gov/EIC/juggler/-/issues/13Track seeding algorithm2021-09-23T15:24:44ZWhitney ArmstrongTrack seeding algorithmAdd generic track seed algo to processing chain.Add generic track seed algo to processing chain.Whitney ArmstrongWhitney Armstrong2020-08-27https://eicweb.phy.anl.gov/EIC/detectors/ip6/-/issues/1Beampipe2021-09-23T15:15:15ZDmitry RomanovBeampipeHere is the latest Beampipe design
[Detector_chamber_201028.stp](/uploads/98764facf5aa545542bde70c78e03667/Detector_chamber_201028.stp)
![image](/uploads/83c48716f78564e4b41d67a3180f9503/image.png)Here is the latest Beampipe design
[Detector_chamber_201028.stp](/uploads/98764facf5aa545542bde70c78e03667/Detector_chamber_201028.stp)
![image](/uploads/83c48716f78564e4b41d67a3180f9503/image.png)https://eicweb.phy.anl.gov/EIC/detectors/ip6/-/issues/8Update the far forward detectors2021-09-23T15:23:40ZWhitney ArmstrongUpdate the far forward detectors![image](/uploads/f0ff2af99483dc5538640282c6c58e7d/image.png)![image](/uploads/f0ff2af99483dc5538640282c6c58e7d/image.png)IP6 beamline and reference detectorWhitney ArmstrongWhitney Armstronghttps://eicweb.phy.anl.gov/EIC/detectors/ip6/-/issues/5The coordinate system2021-09-23T15:18:40ZDmitry RomanovThe coordinate systemInitial direction
- electrons (0, 0, -1)
- p/ions (sin(a), 0, cos(a))
Where (a) is 0.025Initial direction
- electrons (0, 0, -1)
- p/ions (sin(a), 0, cos(a))
Where (a) is 0.025Whitney ArmstrongWhitney Armstronghttps://eicweb.phy.anl.gov/EIC/detectors/ip6/-/issues/31Put beampipe in parallel world.2021-09-20T19:51:40ZWhitney ArmstrongPut beampipe in parallel world.This will help with a few different issues:
1. Acts tracking geometry (layers) near the beam pipe
2. Overlaps -> beampipe should always win.
Need to make sure that it can be swapped between the worlds for overlap checks...This will help with a few different issues:
1. Acts tracking geometry (layers) near the beam pipe
2. Overlaps -> beampipe should always win.
Need to make sure that it can be swapped between the worlds for overlap checks...https://eicweb.phy.anl.gov/EIC/benchmarks/physics_benchmarks/-/issues/3DIS benchmark2023-09-21T19:24:26ZWhitney ArmstrongDIS benchmarkAdd a first DIS benchmark.Add a first DIS benchmark.First Physics Benchmarkhttps://eicweb.phy.anl.gov/EIC/benchmarks/physics_benchmarks/-/issues/4First SIDIS benchmark2023-09-21T19:24:33ZWhitney ArmstrongFirst SIDIS benchmarkPick a SIDIS channel and add a benchmark
Step 1: Generated Q2 spectrum
Step 2: Q2 resolution using reconstructed events
Step 3: Add other inclusive variables
Once this is complete we can start looking at SIDIS.Pick a SIDIS channel and add a benchmark
Step 1: Generated Q2 spectrum
Step 2: Q2 resolution using reconstructed events
Step 3: Add other inclusive variables
Once this is complete we can start looking at SIDIS.First Physics BenchmarkMarshall ScottMarshall Scotthttps://eicweb.phy.anl.gov/EIC/benchmarks/physics_benchmarks/-/issues/19Fix juggler options file2021-09-20T18:31:46ZWhitney ArmstrongFix juggler options fileJob [#154758](https://eicweb.phy.anl.gov/EIC/benchmarks/physics_benchmarks/-/jobs/154758) failed for 2877de0de4d3519f9abf8b1b35d33bea2a66a345:Job [#154758](https://eicweb.phy.anl.gov/EIC/benchmarks/physics_benchmarks/-/jobs/154758) failed for 2877de0de4d3519f9abf8b1b35d33bea2a66a345:Whitney ArmstrongWhitney Armstronghttps://eicweb.phy.anl.gov/EIC/benchmarks/reconstruction_benchmarks/-/issues/17Eta 1.0 - 3.0: Forward detector PID2021-09-23T16:06:31ZWhitney ArmstrongEta 1.0 - 3.0: Forward detector PIDDefine the boundary for PID and transition from TOF to RICH.
![image](/uploads/e524499ee8ffd2d813911a40e208a6ce/image.png)Define the boundary for PID and transition from TOF to RICH.
![image](/uploads/e524499ee8ffd2d813911a40e208a6ce/image.png)Yellow Report Standard DetectorChao PengChao Penghttps://eicweb.phy.anl.gov/EIC/benchmarks/reconstruction_benchmarks/-/issues/6How to do a MR2021-06-09T03:17:35ZWhitney ArmstrongHow to do a MR@sly2j @whit@sly2j @whithttps://eicweb.phy.anl.gov/EIC/juggler/-/issues/15Forward track reconstruction.2023-09-21T19:23:43ZWhitney ArmstrongForward track reconstruction.Forward track reconstruction of low-t events.Forward track reconstruction of low-t events.Whitney ArmstrongWhitney Armstrong2020-07-28https://eicweb.phy.anl.gov/EIC/juggler/-/issues/10PodioInput to PodioOutput2021-09-28T21:38:42ZWhitney ArmstrongPodioInput to PodioOutputJuggler's PodioInput collections are passed to the PodioOutput but they are empty when they are filled.
When passing the input "mcparticles" to the "PodioOutput", or any other input collection, the output collection with the same name i...Juggler's PodioInput collections are passed to the PodioOutput but they are empty when they are filled.
When passing the input "mcparticles" to the "PodioOutput", or any other input collection, the output collection with the same name is empty.Sylvester JoostenSylvester Joosten