This is Nbody6++GPU - Beijing version, an N-body star cluster simulation code, maintained by Rainer Spurzem (spurzem/at/nao.cas.cn) and team.
The code is an offspring of Sverre Aarseth's direct N-body codes see www.sverre.com .
This is the code suitable for parallel and GPU accelerated runs on supercomputers and workstations. Before we give some more practical help, please read the following disambiguation; there is another github of Nbody6++GPU:
LW: https://github.com/nbodyx/ - if interested please contact and collaborate with Long Wang longwang.astro@live.com RS: https://github.com/nbody6ppgpu - if interested please contact and collaborate with Rainer Spurzem spurzem@ari.uni-heidelberg.de spurzem@nao.cas.cn
Here is an example of current differences between the code version (May 2023), more changes and differences may occur in the future, if in doubt, ask the authors.
- LW: implementation of Milky Way potential following the MWPotential2014 in Galpy (Bovy 2015).
- RS: implementation of spin and mass dependent recoil kicks after GW merger (Arca Sedda et al. 2023 subm. MNRAS)
- LW: implementation of python data reading interface for PeTar analysis tool.
- RS: use of HDF5 output files with python data reading interfaces
- RS: Namelist based input format, allowing also to read all stellar evolution and binary / collision parameters.
- LW and RS: Some bug fixes related to Roche and GR radiation, in both versions slightly different ways.
- LW and RS: implementation of BSE from Banerjee et al. 2019
git clone git@github.com:nbody6ppgpu/Nbody6PPGPU-beijing
- This downloads the
stable
branch. Thestable
branch include major versions, and thedev
branch include the most recent updates and bugfix. Changes indev
branch are merged tostable
regularly. - If you want the most recent version (may contain bugs), use
git clone -b dev git@github.com:nbody6ppgpu/Nbody6PPGPU-beijing
, or rungit switch dev
after youclone
without-b dev
param.
./configure --with-par=b1m --enable-simd=sse --enable-mcmodel=large
- If you run NBODY6++GPU on your personal computer or workstation rather than computer clusters, MPI can be disabled by append
--disable-mpi
to the command above. - In the following cases, you may need to append
--disable-gpu
- The computer has no NVIDIA GPU
- The computer has NVIDIA GPU but did not install CUDA compiler (Test: type
nvcc --version
in your terminal. If you see information about NVIDIA compiler, then it is installed. If you see errors like "nvcc: command not found" then it is not installed) - Your simulation has relatively small particle number (< 50000). The code is for up to one million bodies with many initial binaries. In the case of small particle number, GPU can hardly boost the simulation and can sometimes slow it down.
The configure script written by Long Wang has a multitude of further options, check with ./configure --help
or feel free to ask any question in our discussion.
HDF5 is an efficient storage scheme, which is useful during long-time simulations to boost the simulation and save disk spaces. Nevertheless, it is recommended but not necessary. To use HDF5, make sure it is installed in your computer. For example, in Debian based Linux,
apt-get install libhdf5-openmpi-dev
apt-get install libhdf5-dev
after that, append --enable-hdf5
in configure command
make clean ; make -j
After make you find the executable and object files in build/
, named nbody6++.sse.mpi.gpu
. The suffix may change with different compilation options. For example, if you have --disable-mpi --disable-gpu
during configure, the executable may be named nbody6++.sse
- Copy the executable to the simulation directory you want
cp `ls build/nbody6++*` [your_simulation_path]
- Prepare an initial condition file. For a test run, you can find example initial conditions in
examples/input_files
. CopyN100k.inp
anddat.10
to your simulation path
cp examples/input_files/N100k.inp [your_simulation_path]
cp examples/input_files/dat.10 [your_simulation_path]
💡 Starting from the stable version May2023, NBODY6++GPU changes to a fundamentally new and more flexible method of reading input data (control data, not particle data). It uses Fortran NAMELIST input, which has a key=value format. All input data can be given in any order. If you are using a old-format input file, you can use the bash script which transform the old input file into the new one (examples/input_files/@input-transform) to transform it to the new NAMELIST format. See usage inside the script.
- Finally, run it
cd [your_simulation_path]
nbody6++.sse < N100k.inp
Don't forget to replace nbody6++.sse
with the name of your executable
For any further questions, read the documentations at https://www.overleaf.com/read/hcmxcyffjkzq or ask any question in our discussion
git clone -b dev git@github.com:nbody6ppgpu/Nbody6PPGPU-beijing
It would automatically switch to dev branch after downloading.
Sources are in src/Main/
. Due to urgent bug fixes few routines are later than Dec2020.
Git system does not preserve the modification time of files, but the modification time of some ancient files (created before this project was brought to Git) may be valuable information for developers. If you need this info, run python3 restore_mtime.py
after git clone
and each git pull
. It will touch
each file with their real last modification time.
-
The environment variable OMP_NUM_THREADS has to be set to the desired value of OpenMP threads per MPI process. (Maybe your system has it predefined). I also recommend to set OMP_STACKSIZE=4096M the shell where you run the code.
-
It is inefficient (and even more error prone) for particle numbers below about 50k-100k particles (depending on hardware). For smaller N you are advised to disable GPU, or use Nbody6 and Nbody6GPU for single node/process.
-
It is recommended to provide a dat.10 file in N-body input format (see manual). Such file can be produced by other programs, like mcluster.
- https://ui.adsabs.harvard.edu/abs/1999PASP..111.1333A/abstract (Aarseth: NBODY1 to NBODY6)
- https://ui.adsabs.harvard.edu/abs/1999JCoAM.109..407S/abstract (Spurzem on NBODY6++)
- https://ui.adsabs.harvard.edu/abs/2005MNRAS.363..293H/abstract (Hurley+ on SSE/BSE, earlier references therein)
- https://ui.adsabs.harvard.edu/abs/2012MNRAS.424..545N/abstract (Nitadori+: NBODY6GPU)
- https://ui.adsabs.harvard.edu/abs/2015MNRAS.450.4070W/abstract (Wang+: NBODY6++GPU)
- https://ui.adsabs.harvard.edu/abs/2021arXiv210508067K/abstract (Kamlah+: More on current stellar evol.)
-
For systems with more than one GPU on one node the association of MPI rank id and GPU bus id is not well defined, will be improved in next version.
-
Runs with a million or more bodies and huge numbers of binaries (5% or more) use extreme amounts of computing time for the KS binaries (much much more than should be expected). We work on this.
-
On some systems heap and stack management when using OpenMP and MPI together seem to produce very strange errors and segmentation faults. The exact reason is not known; we work on this.
-
Currently using standard OpenMP WITHOUT sse or avx does not work. (it means for configure --disable-simd , but --enable-omp). It uses routines nbint.F instead of special sse or avx routines for neighbour force. We are working on that.
-
Using much more than one million particles (up to ten million) is still not fully supported. configure already allows --with-par=4m , 8m, 10m, b4m, b8m, b10m . Runs of that size may still fail, depending on your hardware and software environment; also the code may still have some glitches (wrong printout, insufficient vector space allocation); test and work is ongoing.
-
Many stellar evolution and other parameters are still compiled into the code (see Table A1 in Kamlah et al. 2022, and parameter FctorCl in Rizzuto et al. 2021), mxns0,1 masses of neutron stars; it is the responsibility of the user to keep them all consistent at compile time (for example mxns and FctorCl are defined in two routines independently, see hrplot, coal, mix). We are working to prepare a nice Fortran NAMELIST style input for ALL parameters (the ones from the current input file, and the ones currently compiled in). That will work like in the style of an .ini file with "key=value" pairs and default values.
-
Currently the use of KZ(7) ge 4 is not working; it produces wrong SIGR2, SIGT2, VROT both in output file and lagr.7. KZ(7) le 3 is ok.
-
For the latest Aug2022 stable version, there may be problems when using some extreme initial conditions (e.g. multiple massive black holes). We work on this.
This code and the documentation is given without warranty, hopefully it is helpful. All may contain errors.