diff --git a/SFEM/README.md b/SFEM/README.md
index 84ebb92dd849ba15b4da3addc22441551c653130..90fb2faef3a82f6fad88928b15626cb1730011fd 100644
--- a/SFEM/README.md
+++ b/SFEM/README.md
@@ -97,48 +97,16 @@ Instructions for Debian/Ubuntu based workstations are as follows.
 * [plotMC.py](./rnnRF/plotMC.py): vizualize the different force displacement curves of the MC simulations.
  * The script reads the simulations results saved in ```'rnnRF/results/RandField_And_GP_X.csv/'```
 
-
-
 ### cellRF
+* [80017_3_128.geo](./cellRF/80017_3_128.geo): geometry file of a lattice cell to be read by gmsh (www.gmsh.info).
+* [80017_3_128.msh](./cellRF/80017_3_128.msh): mesh file of a lattice cell generated by gmsh (www.gmsh.info).
+* [MaterialProperties.csv](./cellRF/MaterialProperties.csv) PA12 viscoelastic-viscoplastic properties, see [MOAMMM cell simulations](https://gitlab.uliege.be/moammm/moammmPublic/syntheticdata/sveresponses).
+* [rve_solver.py](./cellRF/rve_solver.py): interface with cm3Libraries (http://www.ltas-cm3.ulg.ac.be/openSource.htm).
+* [strainPath80017.csv](./cellRF/strainPath80017.csv): loading path applied on the cell, see [MOAMMM cell simulations](https://gitlab.uliege.be/moammm/moammmPublic/syntheticdata/sveresponses).
+* [runthread.py](./cellRF/runthread.py): script to be run to simulate the cell loading case. Deterministic in this example. It requires cm3Libraries (http://www.ltas-cm3.ulg.ac.be/openSource.htm).
 
-Loading paths are generated for three types of loadings:
-
-1. Random Walk paths with rate variant data points (RW).
-2. Random Cyclic paths with rate variant data points (CR).
-3. Random Cyclic paths with constant rate data points (CC).
-
-### rnnRF
-
-Random SVEs are generated for a selected lattice by varying either,the **strut radius** or the **volume fraction**. Geometrical parameters for lattices along with their description are as:
-
-| Parameter |      Type      | Description                                                                            |
-|:----------|:--------------:|:---------------------------------------------------------------------------------------|
-| typeRand  | String literal | Generation parameter for the selected lattice: 'a' for volume fraction, 'b' for radius |
-| vf        | List of floats | Bounds of volume fraction                                                              |
-| rad       |      Int       | Bounds for radius in mm                                                                |
-| size      |  List of int   | Bounds for cell size in mm.                                                            |
-| cell_num  |  list if int   | Periodicity of thr Cell. eg a 1x1x1 cell will be specified as [1, 1, 1]                |
-
-### Material Properties
-
-A visco-elastic - visco-plastic constitutive model [^1] is adopted for data generation. 32 Material Parameters (Incorporating 8 Maxwell Branches) are identified using Bayesian Inference (BI) [^2] for polyamide 12 (PA-12) polymer.
-
-A realization of BI identified material properties, that are provides reliable numerical convergence is used for data generation. These Material parameters are specified in the last row of [PA.csv](./MaterialProperties/PA.csv) and can be selected using the following parameters:
-
-| Parameter |      Type      | Value |
-|:----------|:--------------:|:------|
-| mat       | String literal | "PA"  |
-| mat_ver   |      Int       | 6     |
-
-### Micro-Solver
-
-dG3D micro-solver routines for a macro cauchy continuum or strain gradient continuum can be selected by assigning ```solver``` the value of ```'rve_solver'``` or ```'HO_rve_solver'``` respectively. Furthermore if using higher order kinematics the ```HO``` flag must be set ```True```. 
-
-### Storage Directories
-
-By default, the data is stored as specified in the [Structure of repository](#structure-of-repository). However these paths can be changed using ```load_dir``` and ```data_dir```
 
-## Data Generation
+## Example of application
 
 Once the parameters are defined inside of the driver script, data can be generated. This process consists of three seperate steps: