Changes between Version 1 and Version 2 of jobCards/deuterium

Timestamp:

Jul 25, 2013, 3:23:03 PM (11 years ago)

Author:

jweil

Comment:

switching to TracMathJax? plugin for displaying math

jobCards/deuterium

@@ -19 +19 @@
 $end
 }}}
-Next, we need to define a potential to bind the two nucleons. For this we can't use a mean field, because Deuterium represents a too small system. Instead we use a real two-body potential. Using the parallel ensemble technique, the potential ''V'' for each nucleon in the ''j''th ensemble is given by 
-{{{
-#!latex 
-$V=V_\text{2-body}(r_{1,j}-r_{2,j})$
-}}} 
-where
-{{{
-#!latex 
-$r_{i,j}$
-}}} 
-is the position of the ''i''th nucleon in the ''j''th ensemble. For the full ensemble method, a Deuterium potential is not yet properly implemented. So we choose for the general input and the propagation routines the following switches:
+Next, we need to define a potential to bind the two nucleons. For this we can't use a mean field, because Deuterium represents a too small system. Instead we use a real two-body potential. Using the parallel ensemble technique, the potential ''V'' for each nucleon in the ''j''th ensemble is given by \( V=V_\text{2-body}(r_{1,j}-r_{2,j}) \)
+where \( r_{i,j} \) is the position of the ''i''th nucleon in the ''j''th ensemble. For the full ensemble method, a Deuterium potential is not yet properly implemented. So we choose for the general input and the propagation routines the following switches:
 {{{
 $input