6.3 A summary
Concept links · terms present in this machine draft; source roles are unverified: Lie algebra · adjoint representation · irreducible representation · Lie group · Lie bracket · group homomorphism
To summarize, we have shown that in the three dimensional case we have two distinct Lie groups:
, which geometrically is the space . Its Lie algebra is with Lie bracket the cross-product. We have seen two diferent explicit constructions of , in terms of unit quaternions , and in terms of 2 by 2 unitary matrices of determinant 1 ).
, which has a Lie algebra isomorphic to that of
There is a group homomorphism that takes the first group to the second, which is a two-fold covering map. Its derivative is an isomorphism of the Lie algebras of the two groups.
We can see from these constructions two interesting irreducible representations of these groups:
• A representation on which can be constructed in two diferent ways: as the adjoint representation of either of the two groups, or as the defining representation of This is known to physicists as the “spin representation.
• A representation of the first group on , which is most easily seen as the defining representation of . It is not a representation of since going once around a non-contractible loop starting at the identity takes one to minus the identity, not back to the identity as required. This is called the “spin or “spinor” representation and will be studied in more detail in chapter 7.
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正文:英文 · OCR 机器稿 · 待校对
核对状态:OCR 机器稿 · 待校对
原书 PDF · 印刷页 62、63、64、65、66、67、68、69、70、71、72、73、74
来源版本:2025-10-20
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