Lie theory MOC

Complex matrix Lie algebra

Let 𝐺 βŠ†GL𝑛(β„‚) be a Matrix Lie group, and π’ž denote the set of curves in 𝐺 intersecting identity at zero, i.e.

π’ž={π‘βˆˆπ–¬π–Ίπ—‡πœ”(ℝ,𝐺):𝑐(0)=πŸπ‘›}

The matrix Lie algebra 𝔀 is given by

𝔀={𝑐′(0):π‘βˆˆπ’ž}βŠ†β„‚π‘›Γ—π‘›

i.e. the tangent space at identity, with the Lie bracket given by the Linear commutator:

[𝑋,π‘Œ]=π‘‹π‘Œβˆ’π‘Œπ‘‹
Proof of Lie algebra

By properties of the Linear commutator, βˆ’π‘–[ βˆ’, βˆ’] is alternating bilinear and satisfies the Jacobi identity. All that remains to show is that 𝔀 is closed under this operation. To this end let π‘₯,𝑦 βˆˆπ’ž so that 𝑋 = βˆ’π‘–π‘₯β€²(0) βˆˆπ”€ and π‘Œ = βˆ’π‘–π‘¦β€²(0) βˆˆπ”€. Now define a curve Λœπ‘‹ :ℝ →𝔀 by Λœπ‘‹(𝑑) =𝑦(𝑑) 𝑋 𝑦(𝑑)βˆ’1. Since 𝔀 is a vector space and the Tangent space at any point in a vector space is the vector space, Λœπ‘‹β€²(0) βˆˆπ”€. From the product rule

π‘‘π‘‘π‘‘Λœπ‘‹(𝑑)=𝑦(𝑑)𝑑𝑑𝑑𝑦(𝑑)βˆ’1+𝑦(𝑑)βˆ’1𝑑𝑑𝑑𝑦(𝑑)

and

𝑑𝑑𝑑𝑦(𝑑)𝑦(𝑑)βˆ’1βˆ£π‘‘=0=𝑦(0)𝑑𝑑𝑑𝑦(𝑑)βˆ’1βˆ£π‘‘=0+𝑦(0)βˆ’1𝑑𝑑𝑑𝑦(𝑑)βˆ£π‘‘=0=𝑑𝑑𝑑𝑦(𝑑)βˆ’1βˆ£π‘‘=0+π‘–π‘Œ=0

it follows that 𝑑𝑑𝑑𝑦(𝑑)βˆ’1βˆ£π‘‘=0 = βˆ’π‘–π‘Œ and thus

π‘‘π‘‘π‘‘Λœπ‘‹(𝑑)βˆ£π‘‘=0=𝑦(0)𝑋𝑑𝑑𝑑𝑦(𝑑)βˆ’1βˆ£π‘‘=0+𝑑𝑑𝑑𝑦(𝑑)βˆ£π‘‘=0𝑋𝑦(0)βˆ’1=βˆ’π‘–π‘‹π‘Œ+π‘–π‘Œπ‘‹=βˆ’π‘–[𝑋,π‘Œ]

hence 𝔀 is closed under the Lie bracket.

Basis

A good choice of basis uses coΓΆrdinate lines in a chart containing the identity matrix. Let (π‘ˆ,πœ‘) be a 𝑛-dimensional coΓΆrdinate chart with πœ‘(βƒ—πŸŽ) =𝑒. Then

𝑋𝑖=πœ•πœ•π‘₯π‘–πœ‘βˆ’1(π‘₯1,…,π‘₯𝑛)βˆ£βƒ—π‘₯=βƒ—πŸŽ

See also Lie algebra basis.


#state/tidy | #lang/en | #SemBr