diff --git a/wk/lin_DTT_AB_rho85_PT.m b/wk/lin_DTT_AB_rho85_PT.m
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+%% QUICK RUN SCRIPT
+% This script creates a directory in /results and runs a simulation directly
+% from the Matlab framework. It is meant to run only small problems in linear
+% for benchmarking and debugging purposes since it makes Matlab "busy".
+
+%% Set up the paths for the necessary Matlab modules
+gyacomodir = pwd;
+gyacomodir = gyacomodir(1:end-2);
+% mpirun = 'mpirun';
+mpirun = '/opt/homebrew/bin/mpirun';
+addpath(genpath([gyacomodir,'matlab'])) % Add matlab module
+addpath(genpath([gyacomodir,'matlab/plot'])) % Add plot module
+addpath(genpath([gyacomodir,'matlab/compute'])) % Add compute module
+addpath(genpath([gyacomodir,'matlab/load'])) % Add load module
+
+%% Set simulation parameters
+SIMID = 'lin_DTT'; % Name of the simulation
+RUN = 1; % To run or just to load
+default_plots_options
+EXECNAME = 'gyacomo23_sp'; % single precision
+% EXECNAME = 'gyacomo23_dp'; % double precision
+
+%% Set up physical parameters
+CLUSTER.TIME = '99:00:00'; % Allocation time hh:mm:ss
+NU = 0.05; % Collision frequency
+TAU = 1.0; % e/i temperature ratio
+K_Ne = 1.33; % ele Density '''
+K_Te = 12.0; % ele Temperature '''
+K_Ni = 2.25; % ion Density gradient drive
+K_Ti = 8.25; % ion Temperature '''
+SIGMA_E = 0.0233380; % mass ratio sqrt(m_a/m_i) (correct = 0.0233380)
+NA = 2; % number of kinetic species
+ADIAB_E = (NA==1); % adiabatic electron model
+BETA = 0.0034; % electron plasma beta
+MHD_PD = 0;
+%% Set up grid parameters
+P = 4;
+J = P/2;%P/2;
+PMAX = P; % Hermite basis size
+JMAX = J; % Laguerre basis size
+NX = 32; % real space x-gridpoints
+NY = 16; % real space y-gridpoints
+LX = 2*pi/0.1; % Size of the squared frequency domain in x direction
+LY = 2*pi/0.2; % Size of the squared frequency domain in y direction
+NZ = 32; % number of perpendicular planes (parallel grid)
+SG = 0; % Staggered z grids option
+NEXC = 1; % To extend Lx if needed (Lx = Nexc/(kymin*shear))
+
+%% GEOMETRY
+% GEOMETRY= 's-alpha';
+GEOMETRY= 'miller';
+EPS = 0.28; % inverse aspect ratio
+Q0 = 2.15; % safety factor
+SHEAR = 3.62; % magnetic shear
+KAPPA = 1.53; % elongation
+S_KAPPA = 0.77;
+DELTA = 0.23; % triangularity
+S_DELTA = 1.05;
+ZETA =-0.01; % squareness
+S_ZETA =-0.17;
+PARALLEL_BC = 'dirichlet'; % Boundary condition for parallel direction ('dirichlet','periodic','shearless','disconnected')
+SHIFT_Y = 0.0; % Shift in the periodic BC in z
+NPOL = 1; % Number of poloidal turns
+PB_PHASE = 0;
+%% TIME PARAMETERS
+TMAX = 15; % Maximal time unit
+DT = 1e-3; % Time step
+DTSAVE0D = 1; % Sampling per time unit for 0D arrays
+DTSAVE2D = -1; % Sampling per time unit for 2D arrays
+DTSAVE3D = 2; % Sampling per time unit for 3D arrays
+DTSAVE5D = 100; % Sampling per time unit for 5D arrays
+JOB2LOAD = -1; % Start a new simulation serie
+
+%% OPTIONS
+LINEARITY = 'linear'; % activate non-linearity (is cancelled if KXEQ0 = 1)
+CO = 'DG'; % Collision operator (LB:L.Bernstein, DG:Dougherty, SG:Sugama, LR: Lorentz, LD: Landau)
+GKCO = 1; % Gyrokinetic operator
+ABCO = 1; % INTERSPECIES collisions
+INIT_ZF = 0; % Initialize zero-field quantities
+HRCY_CLOS = 'truncation'; % Closure model for higher order moments
+DMAX = -1;
+NLIN_CLOS = 'truncation'; % Nonlinear closure model for higher order moments
+NMAX = 0;
+KERN = 0; % Kernel model (0 : GK)
+INIT_OPT = 'phi'; % Start simulation with a noisy mom00/phi/allmom
+NUMERICAL_SCHEME = 'RK4'; % Numerical integration scheme (RK2,SSPx_RK2,RK3,SSP_RK3,SSPx_RK3,IMEX_SSP2,ARK2,RK4,DOPRI5)
+
+%% OUTPUTS
+W_DOUBLE = 1; % Output flag for double moments
+W_GAMMA = 1; % Output flag for gamma (Gyrokinetic Energy)
+W_HF = 1; % Output flag for high-frequency potential energy
+W_PHI = 1; % Output flag for potential
+W_NA00 = 1; % Output flag for nalpha00 (density of species alpha)
+W_DENS = 1; % Output flag for total density
+W_TEMP = 1; % Output flag for temperature
+W_NAPJ = 1; % Output flag for nalphaparallel (parallel momentum of species alpha)
+W_SAPJ = 0; % Output flag for saparallel (parallel current of species alpha)
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%% UNUSED PARAMETERS
+% These parameters are usually not to play with in linear runs
+MU = 0.0; % Hyperdiffusivity coefficient
+MU_X = MU; % Hyperdiffusivity coefficient in x direction
+MU_Y = MU; % Hyperdiffusivity coefficient in y direction
+N_HD = 4; % Degree of spatial-hyperdiffusivity
+MU_Z = 2.0; % Hyperdiffusivity coefficient in z direction
+HYP_V = 'hypcoll'; % Kinetic-hyperdiffusivity model
+MU_P = 0.0; % Hyperdiffusivity coefficient for Hermite
+MU_J = 0.0; % Hyperdiffusivity coefficient for Laguerre
+LAMBDAD = 0.0; % Lambda Debye
+NOISE0 = 1.0e-5; % Initial noise amplitude
+BCKGD0 = 0.0e-5; % Initial background
+k_gB = 1.0; % Magnetic gradient strength
+k_cB = 1.0; % Magnetic curvature strength
+COLL_KCUT = 1; % Cutoff for collision operator
+ADIAB_I = 0; % adiabatic ion model
+
+%%-------------------------------------------------------------------------
+%% RUN
+setup
+% system(['rm fort*.90']);
+% Run linear simulation
+if RUN
+ MVIN =['cd ../results/',SIMID,'/',PARAMS,'/;'];
+% RUN =['time ',mpirun,' -np 2 ',gyacomodir,'bin/',EXECNAME,' 1 2 1 0;'];
+% RUN =['time ',mpirun,' -np 4 ',gyacomodir,'bin/',EXECNAME,' 1 2 2 0;'];
+ RUN =['time ',mpirun,' -np 8 ',gyacomodir,'bin/',EXECNAME,' 1 4 2 0;'];
+% RUN =['time ',mpirun,' -np 1 ',gyacomodir,'bin/',EXECNAME,' 1 1 1 0;'];
+ % RUN = ['./../../../bin/gyacomo23_sp 0;'];
+ MVOUT='cd ../../../wk;';
+ system([MVIN,RUN,MVOUT]);
+end
+
+%% Analysis
+% load
+filename = [SIMID,'/',PARAMS,'/']; % Create the filename based on SIMID and PARAMS
+LOCALDIR = [gyacomodir,'results/',filename,'/']; % Create the local directory path based on gyacomodir, results directory, and filename
+FIGDIR = LOCALDIR; % Set FIGDIR to the same path as LOCALDIR
+% Load outputs from jobnummin up to jobnummax
+J0 = 0; J1 = 0;
+data = {}; % Initialize data as an empty cell array
+% load grids, inputs, and time traces
+data = compile_results_low_mem(data,LOCALDIR,J0,J1);
+
+
+if 0 % Activate or not
+%% plot mode evolution and growth rates
+% Load phi
+[data.PHI, data.Ts3D] = compile_results_3D(LOCALDIR,J0,J1,'phi');
+options.NORMALIZED = 0;
+options.TIME = data.Ts3D;
+ % Time window to measure the growth of kx/ky modes
+options.KX_TW = [0.2 1]*data.Ts3D(end);
+options.KY_TW = [0.2 1]*data.Ts3D(end);
+options.NMA = 1; % Set NMA option to 1
+options.NMODES = 999; % Set how much modes we study
+options.iz = 'avg'; % Compressing z
+options.ik = 1; %
+options.fftz.flag = 0; % Set fftz.flag option to 0
+fig = mode_growth_meter(data,options); % Call the function mode_growth_meter with data and options as input arguments, and store the result in fig
+end
+
+if 1
+%% Ballooning plot
+[data.PHI, data.Ts3D] = compile_results_3D(LOCALDIR,J0,J1,'phi');
+if data.inputs.BETA > 0
+[data.PSI, data.Ts3D] = compile_results_3D(LOCALDIR,J0,J1,'psi');
+end
+options.time_2_plot = [120];
+options.kymodes = [0.25];
+options.normalized = 1;
+options.PLOT_KP = 0;
+% options.field = 'phi';
+fig = plot_ballooning(data,options);
+end
+