Table: $c \bar c$ Hybrid Decay Modes
      alt high mass standard IKP reduced
2-+ $ D^{\ast}D $ P .5 .1 .8 4 19
  $D^{\ast \ast}(2^{+})D$ S - 9 - -  
    D - .2 - -  
  $D^{\ast \ast}(1^{+}_L)D$ D - .2 - -  
  $D^{\ast \ast}(0^{+})D$ D - .2 - -  
  $D^{\ast \ast}(1^{+}_H)D$ D - .2 - -  
  $\Gamma$   .5 2 .8 4  
1-+ $ D^{\ast}D $ P .5 .1 .8 4 19
  $D^{\ast \ast}(2^{+})D$ D - .5 - -  
  $D^{\ast \ast}(1^{+}_L)D$ S - 1.2 - -  
    D - 2.5 - -  
  $D^{\ast \ast}(1^{+}_H)D$ S - 25 - -  
    D - 0 - -  
  $\Gamma$   .5 29 .8 4  
0-+ $ D^{\ast}D $ P 2 .3 3 16 76
  $D^{\ast \ast}(2^{+})D$ D - 2.5 - -  
  $D^{\ast \ast}(0^{+})D$ S - 25 - -  
  $\Gamma$   2 28 3 16  
1- $ D^{\ast}D $ P 1 .2 1.5 8 38
  $D^{\ast \ast}(2^{+})D$ D - 1 - -  
  $D^{\ast \ast}(1^{+}_L)D$ S - 7 - -  
    D - .3 - -  
  $D^{\ast \ast}(1^{+}_H)D$ S - 10 - -  
    D - .2 - -  
  $\Gamma$   1 19 1.5 8  
2+- $ D^{\ast}D $ D .2 .2 .3 1 7
  $D^{\ast \ast}(2^{+})D$ P - .5 - -  
    F - .02 - -  
  $D^{\ast \ast}(1^{+}_L)D$ P - 0 - -  
    F - 0 - -  
  $D^{\ast \ast}(1^{+}_H$)D P - 3 - -  
    F - 0 - -  
  $\Gamma$   .2 4 .3 1  
1+- $ D^{\ast}D $ S .3 .1 .5 8 12
    D .1 .1 .1 .5 4
  $D^{\ast \ast}(2^{+})D$ P - 13 - -  
    F - .01 - -  
  $D^{\ast \ast}(1^{+}_L)D$ P - 2 - -  
  $D^{\ast \ast}(0^{+})D$ P - 8 - -  
  $D^{\ast \ast}(1^{+}_H)D$ P - 2.5 - -  
  $\Gamma$   .4 26 .6 8.5  
0+- $D^{\ast \ast}(1^{+}_L)D$ P - 25 - -  
  $D^{\ast \ast}(1^{+}_H)D$ P - 15 - -  
  $\Gamma$   - 40 - -  
1++ $ D^{\ast}D $ S .2 .1 .3 1 6
    D .2 .2 .3 .3 8
  $D^{\ast \ast}(2^{+})D$ P - 5 - -  
    F - .03 - -  
  $D^{\ast \ast}(1^{+}_L)D$ P - 5 - -  
  $D^{\ast \ast}(0^{+})D$ P - Ø - -  
  $D^{\ast \ast}(1^{+}_H)D$ P - 5 - -  
  $\Gamma$   .4 15 .6 1.3  
 



 
Louie Cecil Elliott
1998-08-03