Necessity of bi-invariant metric for Yang-Mill's theory.

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SUMMARY

The necessity of a bi-invariant metric in Yang-Mills theory is established through the action defined as $$ S= \int \frac{1}{4}\text{Tr} (F^{\mu \nu} F_{\mu \nu})d^4 x $$, where the trace is taken with respect to the ad-invariant inner product ##\delta_{kl}##. The discussion confirms that using a non-bi-invariant inner product ##g_{ij}## would compromise gauge invariance, as the transformation $$F_{\mu\nu} \to g F_{\mu\nu} g^{-1}$$ necessitates the preservation of the trace under gauge transformations. Therefore, a bi-invariant inner product is essential for maintaining the gauge invariance of Yang-Mills theory.

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center o bass
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The action for Yang-Mill's theory is often written as
$$ S= \int \frac{1}{4}\text{Tr} (F^{\mu \nu} F_{\mu \nu})d^4 x = \int d^4 x\frac{1}{4} F^{k \mu \nu} F_{k \mu \nu}$$
where latin indices are indicies in the lie algebra, and the trace is taken with respect to the inner product ##\delta_{kl}##. The great thing about this inner product is that it is ad-invariant. I.e. when a gauge transformation is performed ##F\to g F g^{-1}## and
$$\text{Tr} (F^{\mu \nu} F_{\mu \nu}) \to \text{Tr} (g F^{\mu \nu} F_{\mu \nu}g^{-1}) = \text{Tr} (F^{\mu \nu} F_{\mu \nu})$$.

We could imagine implementing more general inner products ##g_{ij}## with the action
$$ S= \int \frac{1}{4} g_{kl} F^{k \mu \nu}, F_{\mu \nu}^l d^4 x$$
that is in general not bi-invariant. Am I wrong that this would destroy the gauge invariance of yang-mills theory? I.e. that gauge theory requires a bi-invariant inner product on ##\mathfrak g##?
 
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Under a gauge transformation, we have

F_{\mu\nu} \to g F_{\mu\nu} g^{-1}
and hence

F^{\mu\nu} F_{\mu\nu} \to g F^{\mu\nu} F_{\mu\nu} g^{-1}
so yes, gauge invariance of the action requires using the bi-invariant metric.
 
center o bass said:
The action for Yang-Mill's theory is often written as
$$ S= \int \frac{1}{4}\text{Tr} (F^{\mu \nu} F_{\mu \nu})d^4 x = \int d^4 x\frac{1}{4} F^{k \mu \nu} F_{k \mu \nu}$$
where latin indices are indicies in the lie algebra, and the trace is taken with respect to the inner product ##\delta_{kl}##. The great thing about this inner product is that it is ad-invariant. I.e. when a gauge transformation is performed ##F\to g F g^{-1}## and
$$\text{Tr} (F^{\mu \nu} F_{\mu \nu}) \to \text{Tr} (g F^{\mu \nu} F_{\mu \nu}g^{-1}) = \text{Tr} (F^{\mu \nu} F_{\mu \nu})$$.

We could imagine implementing more general inner products ##g_{ij}## with the action
$$ S= \int \frac{1}{4} g_{kl} F^{k \mu \nu}, F_{\mu \nu}^l d^4 x$$
that is in general not bi-invariant. Am I wrong that this would destroy the gauge invariance of yang-mills theory? I.e. that gauge theory requires a bi-invariant inner product on ##\mathfrak g##?

See page 12, sec. 4 of the PDF in
https://www.physicsforums.com/showpost.php?p=4238251&postcount=1

Sam
 

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