The equation can be modified to obtain an equation of motion term which contains no covariant derivatives (partial integration):
({(
+
[
,
]),
}+{(
+
[
,
]),
})
=
({![]()
,
}+{![]()
,
})
= -(![]()
+![]()
)
=
-(![]()
+![]()
){
(
+
[
,
] -
)}.
![rh0 = UTrace[NM[UAntiCommutator[hplus[μ][x] + I/2 UCommutator[USmall[μ][x], HLeft[x]], HRight[x]], USmall[μ][x]] + NM[UAntiCommutator[hminus[μ][x] + I/2 UCommutator[USmall[μ][x], HRight[x]], HLeft[x]], USmall[μ][x]]] // NMExpand // Expand](../HTMLFiles/index_255.gif)

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Converted by Mathematica (July 10, 2003)