For expert users

 
Options for the conjugate-gradient algorithm for the computation of the correction potential: rms-convergence (conj-grad conv=1.d-7), maxium number of iteration (maxit=20), output level output=0-3, asymptotic continuation in each iteration (cgasy=1).

With slater-dtresh= 1.d-9 (default) the calculations of the numerical integrals for the Slater potential is performed only if it changes more than 1.d-9.

Asymptotic regions specification:

corrct-region $R_F \; \; \Delta_F$
$0 \ldots R_F-\Delta_F$ : basis-set correction potential
$R_F-\Delta_F \ldots R_F+\Delta_F$ : smooth region
$R_F+\Delta_F \ldots +\infty$ : asymptotic correction
Defaults: $R_F =10$, $\Delta_F=0.5$

slater-region $R_N \; \; \Delta_N \; \; R'_F \; \;\Delta'_F$
$0 \ldots R_N-\Delta_N$ : basis-set Slater potential
$R_N-\Delta_N \ldots R_N+\Delta_N$ : smoothing region
$R_N+\Delta_N \ldots R'_F-\Delta'_F$ : numerical Slater
$R'_F-\Delta'_F \ldots R'_F+\Delta'_F$ : smoothing region
$R'_F+\Delta'_F \ldots +\infty$ : asymptotic Slater
Note: $R'_F-\Delta'_F \le R_F-\Delta_F$
Defaults: $R_N=7$, $\Delta_N=0.5$, $R'_F =10$, $\Delta'_F=0.5$
Use correct-b-region and slater-b-region for the beta spin.