In this folder, the EOS tables were calculated using the TM1e model with L=40 MeV.
The model and paramerer set were described in PRC 90(2014)045802 with L=40 in TABLE II.

We note that the calculation was performed without heavy nuclei and alpha-particles.
Therefore, it is only available at high densities.

Although the dissolution density of heavy nuclei depends on the proton fraction Yp,
it is around Log10(rhob)=14.1 and does not very sensitive to temperature T,
which can be seen from Figs. 1 and 2 of ApJS 197(2011)20.

We provide all quantities of EOS2 with the same definition and form. 
The density range is different from EOS2 due to disappearance of nonuniform matter.
For the case of Yp=0, there is no heavy nuclei and alpha-particles, 
so we calculate from the lowest density for Yp=0.

"rmf4.tab": main table
Log10(rhob) from 14.1 to 16.0 with 20 meshes (different from EOS2);
Log10(T)    from -1.0 to +2.6 with 91 meshes (same as EOS2);
YP          from 0.01 to 0.65 with 65 meshes (same as EOS2);

"rmf4.t00": table for T=0
Log10(rhob) from 14.1 to 16.0 with 20 meshes (different from EOS2);
YP          from 0.01 to 0.65 with 65 meshes (same as EOS2);

"rmf4.yp0": table for Yp=0
Log10(rhob) from  5.1 to 16.0 with 110 meshes(same as EOS2);
Log10(T)    from -1.0 to +2.6 adding T=0 with 92 meshes (same as EOS2);

In order to use the tables rmf4 in numerical calculation, one may input both EOS2 
and rmf4 in numerical code. Then check the fraction of heavy nuclei (X_A) from Log10(rhob)=14.1. 
At X_A=0 (heavy nuclei dissolve), one can replace the data of EOS2 by rmf4.

I apologize that rmf4 is just a rough treatment for the EOS table due to no contributions
from heavy nuclei and alpha-particles. There may be discontinuity at the connection to 
low-density part of EOS2.

In future, we will provide the EOS table including alpha-particles.
We hope to complete a new EOS table covering the whole ranges of T, Yp, and rhob,
where the calculation of nonuniform matter is performed by the self-consistent 
Thomas-Fermi method and the binding energy of alpha-particles depends on T and rhob.