# ====================
# Target Info Table !  From Nadia's iteration: August 2007
# ====================
#  ----- Greated by Zhihong Ye, 09/17/2010
#
# To add comment, make sure the first letter is '#'.
#
# Parameters: 
# A, Z   Target
# R. L   Radiation Length (g/cm^2)
# F(y) parameters AUX(7):
#   RESOL  parameter for DEEPSIG smearing
#   ESEP  = ESEP/1000.0 Separation energy in GeV of target nucleus
#   f0    = f0/1000.0
#   BigB  = BigB/1000.0
#   a     = a/1000.0
#   b     = b/1000.0
#   alpha =
#   
#  Read in Format in FORTRAN: (a6,2i6,2f9.2,6f11.4)
#  If you want to add a target, please follow the exact format of previous targets.
#
#  --- Updated in Dec 27 2012: Update f0, BigB, a, b, alpha, for D2, He3, He4, C12 using E02-019 22Deg Data
#  --- Updated in Dec 30 2012: Update f0, BigB, a, b, alpha, for D2, He3, He4, C12 using E02-019 18Deg Data
#  --- Updated in Mar 12 2013: Update f0, BigB, a, b, alpha, for D2, He3, He4, C12 using XGT2 Data
#  --- Updated in Mar 13 2013: Add f0, BigB, a, b, alpha, for Ca40 Ca48 using XGT2 Data
#  --- Updated in Feb 10 2014: Fit XGT2 Data with Columb Correction
#  --- Updated in Feb 17 2014: Use a heavier mass for He3, +20% more,from 3.016029 to 3.6192348
#  --- Updated in Mar 11 2014: Re-Fitting H2, He3, He4 and C12 with the new XGT2 XS results with CC, He3 with mass+20%
#  --- Updated in May 11 2014: He3 mass is changed back to 100% but with a twist in the model at xbj->3
#  --- Updated in May 16 2014: Re-Fitting all target with the new XGT2 cross section results. 
#  --- Updated in May 19 2014: Remove the twist for He3, add a flat for Fy. 
#  --- Updated in May 20 2014: Re-Fitting all targets. 
#  --- Updated in Nov 07 2016: Add H3 but use He3 values
# -------------------------------------------------------------------------------------------------------
#  Name    A     Z     Mass       R.L.     RESOL     ESEP       f0         BigB        a          b        alpha
# -------------------------------------------------------------------------------------------------------
  H        1     1     1.007940   61.28     0.00     0.0000     5.6000     0.0000     0.0000     0.0000    20.0000
  D2       2     1     2.014102  122.60     0.14     2.2500     9.1884     0.2919     6.1673     6.1293    41.8283
  H3       3     1     3.016049   71.07     0.10     8.4810     4.2222     0.9941     2.6688     8.4550    64.2650 
  He3      3     2     3.016029   71.07     0.10     5.4900     4.2222     0.9941     2.6688     8.4550    64.2650 
  He4      4     2     4.002602   94.32     0.16    20.2000     3.6158     2.4109     2.7674     7.5601   187.4151   
  Be       9     4     9.012182   65.19     0.10     9.2800     3.4814     1.1608     3.1195     7.8398   110.9670
  C       12     6    12.010700   42.70     0.25    17.2700     2.9618     1.9801     3.1402     6.9787   251.3603
  Al      27    13    26.981539   24.01     0.25     9.9000     3.2783     1.3474     2.9698     6.5760   131.8450  
  Ca40    40    20    40.078000   16.14     0.25    10.1569     2.7663     0.9070     3.0546     7.0844   143.1325
  Ca48    48    20    47.952534   16.14     0.25    13.9418     2.5784     1.0295     3.0431     6.8295   168.6328
  Fe      56    26    55.845000   13.84     0.25    10.0600     2.8900     1.4016     3.1802     7.2635   165.7000
  Cu      64    29    63.546000   12.86     0.10     8.5500     2.8740     0.8866     3.0959     7.0945   132.4577
  Au     197    79   196.966569    6.46     0.25     6.9300     2.6424     0.7632     3.0654     6.7678   132.4517