force parameters UNEDF1 corrected

Code/forces.data

@@ -77,9 +77,9 @@
        0.321956, Pairing(232.10945,240.06092,0D0), Pairing(0D0,0D0,0D0)),  &  ! power,VDI,DDDI
        !*************************************************************************
        Force('UNEDF1',1,-1,  (/20.73553,20.73553/),  & ! Name,ex,zpe,h2m
-       -2078.328,239.401,1574.243,14263.646,76.736,  & ! t0,t1,t2,t3,t4
-       0.54304371E-01,-5.0781477    ,-1.3665705    ,-.16116885  ,71.31652,  & !x0,x1,x2,x3,b4p
-       0.270018, Pairing(253.09138,258.11805,0D0), Pairing(0D0,0D0,0D0)),  & ! power,VDI,DDDI
+       -2078.32802326,239.40081204,1575.11954190,14263.64624708,76.73614412,  & ! t0,t1,t2,t3,t4
+       0.5375692E-01,-5.07723238,-1.36650561,-0.16249117,71.3165223,  & !x0,x1,x2,x3,b4p
+       0.27001801, Pairing(253.09138,258.11805,0D0), Pairing(0D0,0D0,0D0)),  & ! power,VDI,DDDI
        !*************************************************************************
        Force('TOV',1,1,  (/20.73553,20.73553/),  & ! Name,ex,zpe,h2m
        -2129.734632,305.3978920,362.5321529,13957.06425,74.14713700,  & !  t0,t1,t2,t3,t4

Code/forces.f90

@@ -161,7 +161,7 @@ CONTAINS
     ENDIF
     ! turn off zpe if desired
     IF(turnoff_zpe) THEN
-       f%zpe=1
+       f%zpe=-1
        WRITE(*,*) '***** Zero-point-energy correction turned off'
     END IF
     ! calculate "b" and Slater coefficients

Paper/v1.1/update.tex

@@ -250,11 +250,11 @@ found as {\tt update.pdf} in the {\tt Documentation} subdirectory.
   execute {\tt make html}, {\tt make latex}, or {\tt make all} to
   produce the corresponding version or both of them.
 
-{\color{red}
+%{\color{red}
   The documentation inserted into the source files accounts for most
   of the formal changes in them. The general documentation is also
   updated and present as ``Documentation.pdf''.
-}
+%}
 
  {\bf Bug fixes:} 
 \begin{enumerate}
@@ -268,14 +268,14 @@ found as {\tt update.pdf} in the {\tt Documentation} subdirectory.
   analysis was activated only for {\tt nof}>1 such that it was absent
   after restart.
 
-{\color{red}
+%{\color{red}
 \item In the time-dependent mode, the wave functions were only save at
   intervals of {\tt mprint} and {\tt mrest}, respectively. If a
   calculation stops because of reaching the final distance or
   fulfilling the convergence criterion, this may lead to a loss of
   information, so that now both are done also in this event before the
   job finishes.
-}
+%}
 
 \item The external field parameters were calculated directly from the
   input in {\tt getin\_external}. Since this is called before the
@@ -374,7 +374,7 @@ expectation value by this factor.  Note that if the external field is
 composed of a mixture of different multipoles (not coded presently),
 an overall scale factor should instead be used.
 
-{\color{red}
+%{\color{red}
 {\bf Enhanced two-body analysis:} the analysis of the final two-body
 quantities after breakup included directly in the code was very
 simplified and actually it was superfluous to do this so frequently.
@@ -384,7 +384,7 @@ a quite accurate Coulomb energy. It is done only when the final
 separation is reached, while a simple determination of whether the
 fragments have separated and, if so, what their distance is, is
 performed every time step.
-}
+%}
 
  {\bf Diagonalization} In the original program the diagonalization of
  the Hamiltonian in the subroutine {\tt diagstep} was carried out