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Commit 4620942f authored by Antoine Cyril David Hoffmann's avatar Antoine Cyril David Hoffmann
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Separation between road map (future) and changelog (past)

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......@@ -11,59 +11,64 @@ How to run it
// Comment : For some collision operators (Sugama and Full Coulomb) you have to run COSOlver from B.J.Frei first in order to generate the required matrices in HeLaZ/iCa folder.
# Road map
(Current version : 2.5)
# Changelog
0. Write MOLI matlab solver in Fortran using Monli1D as starting point
2. MPI parallel version
0.0 go from 1D space to 2D fourier and from Hermite basis to Hermite-Laguerre basis
>2.5 GK Sugama collision operator
0.1 implement linear Poisson equation in fourier space
2.4 2D cartesian parallel (along p and kr)
0.2 implement moment hierarchy linear terms
2.3 GK Dougherty operator
0.3 RK4 time solver
2.2 Allow restart with different P,J values (results are not concluents)
0.4 Benchmark with MOLI matlab results for Z-pinch (cf. kz_linear script)
2.1 First compilable parallel version (1D parallel along kr)
0.5 Load COSOlver matrices
1. Implementation of the non linear Poisson brackets term
0.6 Benchmarks now include Dougherty, Lenard-Bernstein and Full Coulomb collision operators
1.4 Quantitative study with stationary average particle flux \Gamma_\infty
1. Implementation of the non linear Poisson brackets term
1.3 Linear analysis showed that a certain amount of PJ are recquired to trigger mode
1.0 FFTW3 has been used to treat the convolution as a product and discrete fourier transform
1.2 Zonal flows are observed in a similar way to Ricci Rogers 2006 with GS2
1.1 Qualitative test : find similar turbulences as Hasegawa Wakatani system with few moments
1.1 Methods in fourier_mod.f90 have been validated by tests on Hasegawa Wakatani system
1.1 Qualitative test : find similar turbulences as Hasegawa Wakatani system with few moments
1.1 Methods in fourier_mod.f90 have been validated by tests on Hasegawa Wakatani system
1.2 Zonal flows are observed in a similar way to Ricci Rogers 2006 with GS2
1.0 FFTW3 has been used to treat the convolution as a product and discrete fourier transform
1.3 Linear analysis showed that a certain amount of PJ are recquired to trigger mode
0. Write MOLI matlab solver in Fortran using Monli1D as starting point
1.4 Quantitative study with stationary average particle flux \Gamma_\infty
0.6 Benchmarks now include Dougherty, Lenard-Bernstein and Full Coulomb collision operators
2. MPI parallel version
0.5 Load COSOlver matrices
2.1 First compilable parallel version (1D parallel along kr)
0.4 Benchmark with MOLI matlab results for Z-pinch (cf. kz_linear script)
2.2 Allow restart with different P,J values (results are not concluents)
0.3 RK4 time solver
2.3 GK Dougherty operator
0.2 implement moment hierarchy linear terms
2.4 2D cartesian parallel (along p and kr)
0.1 implement linear Poisson equation in fourier space
0.0 go from 1D space to 2D fourier and from Hermite basis to Hermite-Laguerre basis
>2.5 GK Sugama collision operator
# Roadmap
2. MPI parallel version
2.6 GPU accelerated version
2.7 GK Full Coulomb collision operator
4. GK 3D version, kr,kz,kpar for linear device
3. GK 3D version, kr,kz,kpar for linear device
5. DK 3D version, kr,kz,kpar for linear device
4. DK 3D version, kr,kz,kpar for linear device
6. DK+GK 3D version, kr,kz,kpar for linear device
5. DK+GK 3D version, kr,kz,kpar for linear device
7. 3D version with curvature
6. 3D version with curvature
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