The equation can be modified to obtain an equation of motion term which contains no covariant derivatives (partial integration):
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+
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- (
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![rh0 = UTrace[NM[hminus[μ][x] + I/2 UCommutator[USmall[μ][x], HRight[x]], HRight[x], USmall[μ][x]] + NM[HLeft[x], hplus[μ][x] + I/2 UCommutator[USmall[μ][x], HLeft[x]], USmall[μ][x]] - NM[hplus[μ][x] + I/2 UCommutator[USmall[μ][x], HLeft[x]], HLeft[x], USmall[μ][x]] - NM[HRight[x], hminus[μ][x] + I/2 UCommutator[USmall[μ][x], HRight[x]], USmall[μ][x]]] // NMExpand // Expand](../HTMLFiles/index_248.gif)

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Converted by Mathematica (July 10, 2003)