Sorry for my precedent tentative, I was a little hasty:
Ok, I think I'd better put the original problem:
I have an action of three fields: $A$ which is the spin-connection, $B$ an skew-symmetric 2-form and $Phi$ which is traceless and skew-symmetric scalar field. These fields take their values on some algebra, index their components in this algebra by $i,j,k,... = 1,2,3$
I want to implement a certain condition on B by using equations of motion of $Phi$, the action is:
$S=int (B_i wedge F^i + Lambda B_i wedge B^i + Phi_{ij} B^i wedge B^j) $
Now for me equations of motions are simply:
$B^i wedge B^j=0$
perhaps with the condition that all diagonal elements are equal (as jc showed) but this is automatically satisfied for a skew-symmetric matrix (here $B^i wedge B^j$).
But in all papers I find:
$B^i wedge B^j - frac{1}{3}delta^{ij}B_kwedge B^k = 0$
So I see that they all took the traceless part of the matrix representing equations of motion, necessarily it has a relation with the traceless character of $Phi$ but I do not see which one.
In addition, this expression is not antisymmetric in $i,j$.
Would anyone have an idea?
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