Lie Algebras
The Lie algebra $\mathfrak{g}$ is the tangent space to the Lie group $G$ at the identity. It is a vector space equipped with a bracket $[\cdot,\cdot]$ that captures the non-commutativity of the group. For physicists, the generators are the observables — charge, angular momentum, color — and their commutation relations determine the entire representation theory.
Key Concepts
Key Equations
Structure Constants of
The generators of are . Using the known Pauli matrix commutator , find .
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From the definition : .
Comparing: , so .
More generally, for (the Levi-Civita symbol).
Exercises
7 problemsFor generators with , what is ?
The rank of is . What is the rank of ?
For , the normalization gives . What is ?
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Upgrade to Pro →How many generators does have?
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Upgrade to Pro →Structure constants are totally antisymmetric: . If for , what is ?
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Upgrade to Pro →How many generators does have? ( has generators.)
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Upgrade to Pro →How many diagonal Gell-Mann matrices are there? (Equals the rank of .)
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Upgrade to Pro →Key Takeaways
- The Lie algebra is the tangent space at the identity of . It is a vector space with a bracket encoding the local structure of the group.
- Structure constants defined by are totally antisymmetric and satisfy the Jacobi identity.
- For : (angular momentum algebra). For : 28 independent non-zero .
- The rank of is : the number of simultaneously diagonalizable generators (conserved, commuting charges).