afterburner

EIC MC afterburner. Software package to provide framework independent well validated crossing angle and beam effects C++ library and HepMC file converter (abconv) for Electron Ion Collider.

Physics simulated:

• Crossing angle
• Beam effects (divergence, crabbing kick, etc.)
• Vertex spread (position, time)

Software:

• Standalone framework independent code
• Clean C++ API to embed in analysis scripts and/or frameworks
• Convenient Command Line Interface (CLI) HepMC2/3 and root.hepmc converter, that adds crossing_angle_hor and beam effects
• Configurable beam parameters interface (yaml files)

Installation

The converter and benchmark require libyaml-cpp. Those are available in package managers for the most of systems:

apt install libyaml-cpp-dev     # Debian/Ubuntu/Mint
yum install yaml-cpp-devel      # RHEL/CentOS/Fedora

git clone https://eicweb.phy.anl.gov/monte_carlo/afterburner.git
mkdir -p afterburner/build
cd afterburner/build

# setup cmake (c++ code lives in cpp directory) 
cmake ../cpp

# to build all
cmake --build ../cpp --target all

# to install
cmake --build ../cpp --target install -- -j 8

Preinstalled versions are available in ATHENA containers.

CLI command

Examples:

# Process my whole file, add crossing angle, beam effects, do validation plots
abconv my.hepmc

# Same, but limit the number of events to 1000 and set the output name as 'test'
abconv my.hepmc -o test -l 1000

# Just convert hepmc3 to hepmc2 don't use afterburner, don't create plots
abconv my.hepmc -f hepmc2 --ab-off --plot-off 

# Just convert hepmc3 to hepmc.root don't use afterburner, don't create plots
abconv my.hepmc -f treeroot --ab-off --plot-off 

Note: In the final example above, you want the treeroot option. The root option creates a (rather strange) flat file.

How exactly the afterburner works illustrated by abconv my.hepmc command.

Afterburner algorithm

1. AB opens the input file, gets beam particles and extract beam energy settings (from the first event). See beam energy settings for the details below.

2. AB awaits that there is no crossing angle between beam particles. To check this AB calculates a crossing angle between the beam particles. If the crossing angle is not zero and --exit-ca flag is set - AB exits; without the flag a warning is issued.

3. AB processes events applying crossing angle and beam effects for each event. -s,--ev-start, -e,--ev-end, -l,--limit flags limit the number of events to process

4. By defaults AB also creates *.hist.root file that contains validation histograms
   --plot-off flag can switch off histograms creation

P.S. Is one needs just HepMC3->HepMC2 converter one can use --ab-off flag to disable afterburner during conversion. This way abconv could be use as different HepMC formats converter.

Beam energy settings

• The input file events must have two beam particles (marked by status code 4)
• Beam particle energies should correspond to one of EIC beam energy setups:
  • ep [GeV]: 275x18, 275x10, 100x10, 100x5, 41x5
  • eAu [GeV]: 110x18, 110x10, 110x5, 41x5
• One can the exact beam parameters that correspond to EIC CDR tables 3.3, 3.4, 3.5
• Using -p/--preset flag one can select a profile:
  • 0: IP6 High Divergence (higher luminosity) - default,
  • 1: IP6 High Acceptance
  • 2: IP6 eAu
  • 3: IP8 High Divergence (higher luminosity) - default,
  • 4: IP8 High Acceptance
  • 5: IP8 eAu
• Crossing angle is given in horizontal and vertical components
  • Afterburner configuration

(!) For now IP8 is a copy of IP6 parameters with 35 mrad crossing angle. It will be populated with IP8 own parameters as soon as they are officially published.

Input file requirements

• The CLI command can accept any file, that HepMC3 library can open: HepMC3 ascii, HepMC2 ascii, HepMC3 ROOT, HepEvt etc.
• The input file events must have two beam particles (marked by status code 4)
• Input file should not have crossing angle and beam effects that AB simulates. By default, it is not possible to apply just crossing angle or just beam effects. But! in the upcoming version one can provide beam parameters through yaml config files, where one would be able to switch off crossing angle, beam effects, etc.

All options:

Flag	Description
-h,--help	Print this help message and exit
-v,--version	Shows package version number
-o,--output TEXT	Base name for Output files ((!) no extension)
-p,--preset TEXT	Beams configuration 0: IP6 High divergence[default], 1: IP6 High acceptance, 2: IP6 eAu
-i,--in-format TEXT	Input format: auto [default], hepmc2, hepmc3, hpe, lhef, gz, treeroot, root
-f,--out-format TEXT	Output format: hepmc3 [default], hepmc2, dot, none (no events file is saved)
-s,--ev-start INT	Start event index (all previous are skipped)
-e,--ev-end INT	End event index (end processing after this event)
-l,--limit UINT	Limit number of events to process. (Shutdown after this number of parsed events)
--ab-off	No afterburner is applied
--plot-off	Don't produce validation plots
--exit-ca	Check existing crossing angle and exit if CA>1mrad (1)

(1) How --exit-ca works exactly: when afterburner processes the first event it checks if it has 2 beam particles (fails with non zero code if not) and then calculates their crossing angle with the --exit-ca is set and crossing angle absolute value is > 1mrad program ends with 0 code. This method is very coarse as if in a source file the crossing angle is 0 but all beam effects do exist, beam effects will be applied twice

-p,--preset flag, values [0,1,2,3,4,5] set config and auto determine energy from source file:

• "0": IP6, High divergence, auto read energy [default],
• "1": IP6, High acceptance, auto read energy
• "2": IP6, eAu, auto read energy
• "3": IP8, High divergence, auto read energy [default],
• "4": IP8, High acceptance, auto read energy
• "5": IP8, eAu, auto read energy

The other options sets energy settings manually, not checking the source file:

ip6_hidiv_41x5	ip6_hidiv_100x5	ip6_hidiv_100x10	ip6_hidiv_275x10	ip6_hidiv_275x18
ip6_hiacc_41x5	ip6_hiacc_100x5	ip6_hiacc_100x10	ip6_hiacc_275x10	ip6_hiacc_275x18
ip6_eau_41x5	ip6_eau_110x5	ip6_eau_110x10	ip6_eau_110x18	-
ip8_hidiv_41x5	ip8_hidiv_100x5	ip8_hidiv_100x10	ip8_hidiv_275x10	ip8_hidiv_275x18
ip8_hiacc_41x5	ip8_hiacc_100x5	ip8_hiacc_100x10	ip8_hiacc_275x10	ip8_hiacc_275x18
ip8_eau_41x5	ip8_eau_110x5	ip8_eau_110x10	ip8_eau_110x18	-

Example of manual configuration setting:

abconv -p ip6_hidiv_100x5 source_file.hepmc

(!) For now IP8 is a copy of IP6 parameters with 35 mrad crossing angle. It will be populated with IP8 own parameters as soon as they are officially published.

Validation

The validation is performed by comparison of the resulting particle distributions with Pythia8 beam effects simulation. The later was also validated with Fun4All afterburner implementation.

To apply benchmarks. Head-on data (no crossing angle nor effects) is located:

https://eics3.sdcc.bnl.gov:9000/minio/eictest/ATHENA/WG/BeamEffects/

The validation plots are generated and can be viewed in python/comparison.ipynb

Essential plots from the latest validation run:

The discrepancy in low Eta has been explained by a slight phase space difference in generated headon and full beam effects files on Pythia8 side. TL;DR; It is Fine

41x5 GeV	100x10 GeV	275x18 GeV

References

• Accelerator and beam conditions critical for physics and detector simulations for the Electron-Ion Collider
• Pythia8 beam effects
• Fun4All code