Skip to content
Snippets Groups Projects
Commit 74a74cfa authored by Antoine Cyril David Hoffmann's avatar Antoine Cyril David Hoffmann 🌱
Browse files

Update README.md

parent a3755fc2
No related branches found
No related tags found
No related merge requests found
......@@ -64,82 +64,79 @@ Note: For some collision operators (Sugama and Full Coulomb), you will need to r
# Changelog
### 4.x GYACOMO
### v3.x GYACOMO
> installation tutorials and python analysis scripts (SPC release)
>4.11 background ExB shear
> background ExB shear
>4.1 Miller geometry benchmarked
> Miller geometry benchmarked
>4.01 Singular value decomposition is availale with LAPACK (used for DLRA experiments)
> singular value decomposition is availale with LAPACK (used for DLRA experiments)
>4.0 Gyacomo is born and the code is open-source with a GNU GPLv3 license
> Gyacomo is born and the code is open-source with a GNU GPLv3 license
### 3.x HeLaZ 3D (flux tube s-alpha)
### v2.x HeLaZ 3D (flux tube s-alpha)
>3.9 Perpendicular electromagnetic fluctuations by solving Ampere equations (benchmarked linearly)
> perpendicular electromagnetic fluctuations by solving Ampere equations (benchmarked linearly)
>3.8 Benchmarked for CBC against GENE for various gradients values (see Dimits_fig3.m)
> benchmarked for CBC against GENE for various gradients values (see Dimits_fig3.m)
>3.7 The frequency plane has been transposed from positive kx to positive ky for easier implementation of shear. Also added 3D Z-pinch geometry
> transpose the frequency plane from positive kx to positive ky for easier implementation of shear. Also added 3D Z-pinch geometry
>3.6 MPI 3D parallelization in p, kx and z and benchmarked for each parallel options with gbms (new molix) for linear fluxtube shearless.
> MPI 3D parallelization in p, kx and z and benchmarked for each parallel options with gbms (new molix) for linear fluxtube shearless.
>3.5 Staggered grid for parallel odd/even coupling
> staggered grid for parallel odd/even coupling
>3.4 Adiabatic electrons
> adiabatic electrons
>3.3 Benchmarked in fluxtube s-alpha geometry linear run with molix (B.J.Frei) code and works now for shear = 0 with periodic z BC
> benchmarked in fluxtube s-alpha geometry linear run with molix (B.J.Frei) code and works now for shear = 0 with periodic z BC
>3.2 Stopping file procedure like in GBS is added
> stopping file procedure like in GBS is added
>3.1 Implementation of mirror force
> implementation of mirror force
>3.0 3D version and works as the 2D version if Nz = 1, the coordinates were renamed from (r,z) to (x,y,z). Now the parallel direction is ez.
> 3D version and works as the 2D version if Nz = 1, the coordinates were renamed from (r,z) to (x,y,z). Now the parallel direction is ez.
### 2.x 2D Zpinch MPI parallel version
### v1.x 2D Zpinch MPI parallel version
>2.7 Versatile interpolation of kperp for the cosolver matrices and corrections done on DGGK
> versatile interpolation of kperp for the cosolver matrices and corrections done on DGGK
>2.6 Change of collisionality normalisation (from nu_ei to nu_ii), implementation of FCGK
> change of collisionality normalisation (from nu_ei to nu_ii), implementation of FCGK
>2.5 GK cosolver collision implementation
> GK cosolver collision implementation
>2.4 MPI 2D cartesian parallel (along p and kr)
> MPI 2D cartesian parallel (along p and kr)
>2.3 GK Dougherty operator
> GK Dougherty operator
>2.2 Allow restart with different P,J values
> allow restart with different P,J values
>2.1 First compilable parallel version (1D parallel along kr)
> first compilable parallel version (1D parallel along kr)
### 1.x Implementation of the non linear Poisson bracket term
### v0.x Implementation of the non linear Poisson bracket term
>1.4 Quantitative study with stationary average particle flux \Gamma_\infty
> 1uantitative study with stationary average particle flux \Gamma_\infty
>1.3 Linear analysis showed that a certain amount of PJ are recquired to trigger mode
> linear analysis showed that a certain amount of PJ are recquired to trigger mode
>1.2 Zonal flows are observed in a similar way to Ricci Rogers 2006 with GS2
> zonal flows observed, qualitative agreement with Ricci et al. 2006 (GS2)
>1.1 Qualitative test : find similar turbulences as Hasegawa Wakatani system with few moments
> 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
> methods in fourier_mod.f90 have been validated by tests on Hasegawa Wakatani system
>1.1 Methods in fourier_mod.f90 have been validated by tests on Hasegawa Wakatani system
> FFTW3 has been used to treat the convolution as a product and discrete fourier transform
>1.0 FFTW3 has been used to treat the convolution as a product and discrete fourier transform
> load COSOlver matrices
### 0.x Write MOLI matlab solver in Fortran using Monli1D as starting point
> benchmark with MOLI matlab results for Z-pinch (cf. kz_linear script)
>0.6 Benchmarks now include Dougherty, Lenard-Bernstein and Full Coulomb collision operators
> RK4 time solver
>0.5 Load COSOlver matrices
> implement moment hierarchy linear terms
>0.4 Benchmark with MOLI matlab results for Z-pinch (cf. kz_linear script)
> implement linear Poisson equation in fourier space
>0.3 RK4 time solver
> go from 1D space to 2D fourier and from Hermite basis to Hermite-Laguerre basis
>0.2 implement moment hierarchy linear terms
>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
> start from GBS skeleton
\ No newline at end of file
0% Loading or .
You are about to add 0 people to the discussion. Proceed with caution.
Finish editing this message first!
Please register or to comment