$\delta \epsilon^{(1)}$   $\delta \epsilon$           $\delta          Other
                                                                                           \epsilon_{\rm Br, fit}$  
  ------ ------------ --------------------- ------------------------- ------------------- ------------------------- ------------------------------------------
  Na     $3s_{1/2}$         -0.182033             -5.559\[-7\]           -5.910\[-7\]           -6.701\[-7\]        -6.016\[-7\]

         $3p_{1/2}$         -0.109490             -2.006\[-10\]           3.067\[-8\]            3.537\[-8\]        

         $3p_{3/2}$         -0.109417             -4.101\[-11\]           3.077\[-8\]            3.548\[-8\]        

         $3d_{3/2}$         -0.055667             -6.538\[-18\]          -1.323\[-10\]          -1.412\[-10\]       

         $3d_{5/2}$         -0.055667             -2.018\[-18\]          -1.347\[-10\]          -1.439\[-10\]       

  K      $4s_{1/2}$         -0.147491             -1.224\[-6\]           -1.333\[-6\]           -1.717\[-6\]        -1.371\[-6\]

         $4p_{1/2}$         -0.095713             -1.879\[-9\]            7.262\[-8\]            9.376\[-8\]        

         $4p_{3/2}$         -0.095498             -3.547\[-10\]           7.396\[-8\]            9.524\[-8\]        

         $3d_{3/2}$         -0.058067             -1.046\[-14\]           1.395\[-8\]            4.172\[-8\]        

         $3d_{5/2}$         -0.058080             -3.112\[-15\]           1.376\[-8\]           4.125\[-8 \]        

  Rb     $5s_{1/2}$         -0.139291             -4.648\[-6\]           -5.114\[-6\]           -6.767\[-6\]        -5.288\[-6\]

         $5p_{1/2}$         -0.090816             -3.234\[-8\]            1.776\[-7\]            2.365\[-7\]        

         $5p_{3/2}$         -0.089986             -4.881\[-9\]            2.108\[-7\]            2.774\[-7\]        

         $4d_{3/2}$         -0.059687             -3.865\[-12\]           1.290\[-7\]            3.184\[-7\]        

         $4d_{5/2}$         -0.059745             -1.048\[-12\]           1.218\[-7\]            3.001\[-7\]        

  Cs     $6s_{1/2}$         -0.127368             -1.054\[-5\]           -1.160\[-5\]           -1.583\[-5\]        -1.206\[-5\], -1.054\[-5\], -1.159\[-5\]

         $6p_{1/2}$         -0.085616             -1.942\[-7\]            2.288\[-7\]            3.168\[-7\]        -1.942\[-7\], 2.284\[-7\]

         $6p_{3/2}$         -0.083785             -2.178\[-8\]            4.518\[-7\]            6.097\[-7\]        -2.180\[-8\], 4.513\[-7\]

         $5d_{3/2}$         -0.064420             -1.938\[-10\]           1.127\[-6\]            2.516\[-6\]        

         $5d_{5/2}$         -0.064530             -4.612\[-11\]           1.007\[-6\]            2.216\[-6\]        

  Fr     $7s_{1/2}$         -0.131076             -4.997\[-5\]           -5.540\[-5\]           -7.227\[-5\]        -5.828\[-5\]

         $7p_{1/2}$         -0.085911             -2.569\[-6\]           -1.610\[-6\]           -2.414\[-6\]        

         $7p_{3/2}$         -0.080443             -1.356\[-7\]            1.834\[-6\]            2.408\[-6\]        

         $6d_{3/2}$         -0.062993             -3.579\[-9\]            3.822\[-6\]            8.765\[-6\]        

         $6d_{5/2}$         -0.063444             -6.921\[-10\]           2.606\[-6\]            5.720\[-6\]        

  E119   $8s_{1/2}$         -0.152842             -3.427\[-4\]           -4.046\[-4\]           -4.484\[-4\]        -4.436\[-4\]

         $8p_{1/2}$         -0.091697             -3.921\[-5\]           -4.701\[-5\]           -7.643\[-5\]        

         $8p_{3/2}$         -0.075972             -5.420\[-7\]            1.120\[-5\]            1.430\[-5\]        

         $7d_{3/2}$         -0.061414             -2.517\[-8\]            8.715\[-6\]            2.594\[-5\]        

         $7d_{5/2}$         -0.063000             -4.420\[-9\]           -1.374\[-6\]            9.042\[-7\]        
  ------------------------------------------------------------------------------------------------------------------------------------------------------------

The effect of the correlation potential is to pull the wave functions closer to 