Anomaly Cancellation for GUTS: Beginner's Questions

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Anomaly cancellation in Grand Unified Theories (GUTs) is crucial for maintaining local gauge invariance, as anomalies that break this invariance render the theory inconsistent. While global symmetries can have anomalies without significant issues, local gauge invariance is essential both theoretically and experimentally. To address potential anomalies, physicists have developed consistency equations to ensure that anomalous terms are counterbalanced by other terms. Certain Lie groups, such as SO(10), inherently provide anomaly-free representations, while GUTs with additional U(1) factors require careful consideration. Thus, anomaly cancellation is more of a mathematical requirement than an axiom in the context of GUTs.
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Beginners question :

In GUTS what is the relevance of anomaly cancellation.

Is it in some sense an axiom - like we say we must have local invariance - or is it in just some mathematical requirement?

Thanks in advance.
 
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We don't care too much about global symmetries being anomalous, for instance the axial anomaly of QCD.

Otoh if we have anomalies that break local gauge invariance, we have a serious problem, the theory is necessarily inconsistent (both theoretically and by experiment, gauge invariance is key). So people devised consistency equations to ensure that anomalous terms were matched with other (often adhoc) terms that precisely cancel.

Now as far as GUTs go, some lie groups furnish anomaly free irreps automatically (eg SO(10)), its usually the GUTs with extra U(1) factors lying around that you ahve to be careful with.
 
So its not really an axiom - more a requirement.
 

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