Lie theory MOC

Haar measure of a compact Lie group

Let 𝐺 be an 𝑛-dimensional Compact Lie group, 𝔀 be its corresponding Lie algebra1 with basis {𝑋𝑗}𝑛𝑗=1, and (π‘ˆ,πœ‘) be a coΓΆrdinate chart with πœ‘(𝑒) =βƒ—πŸŽ. For each πœ‘(π‘₯) βˆˆπ‘ˆ βŠ†πΊ define π΄πœ‘π‘—π‘˜(π‘₯) so that

βˆ’π‘–πœ‘βˆ’1(π‘₯)βˆ’1πœ•π‘—πœ‘βˆ’1(π‘₯)=π‘›βˆ‘π‘˜=1π‘‹π‘˜π΄πœ‘π‘˜π‘—(π‘₯)

where both sides are clearly elements of 𝔀. Then for any Borel set 𝐡 βŠ†π‘ˆ, the unique left and right Haar measure πœ‡(𝐡) is given by #m/thm/group

πœ‡(𝐡)=βˆ«π΅π‘‘πœ‡(𝑔)=βˆ«πœ‘(𝐡)𝛼|detπ€πœ‘(π‘₯)|𝑑𝑛π‘₯

where 𝛼 is a normalisation constant. The Haar measure is defined for the whole of 𝐺 by translating the chart (enabled by invariance).

Proof this is a Haar measure

Let (𝑉,πœ“) define a chart with π‘ˆ βˆ©π‘‰ β‰ βˆ…, and let 𝑓 be a transition map such that πœ“(π‘₯) =πœ‘(𝑓(π‘₯)) for all π‘₯ βˆˆπœ“(π‘ˆ βˆ©π‘‰). Then

π‘›βˆ‘π‘˜=1π‘‹π‘˜π΄πœ“π‘˜π‘—(π‘₯)=βˆ’π‘–πœ“βˆ’1(π‘₯)βˆ’1πœ•π‘—πœ“βˆ’1(π‘₯)=βˆ’π‘–[πœ‘βˆ’1βˆ˜π‘“](π‘₯)βˆ’1πœ•π‘—[πœ‘βˆ’1βˆ˜π‘“](π‘₯)=βˆ’π‘–[πœ‘βˆ’1βˆ˜π‘“](π‘₯)βˆ’1π‘›βˆ‘β„“=1πœ•π‘—π‘“β„“(π‘₯)[πœ•β„“πœ‘βˆ’1βˆ˜π‘“](π‘₯)=π‘›βˆ‘β„“,π‘˜=1π‘‹π‘˜π΄πœ‘π‘˜β„“(𝑓(π‘₯))πœ•π‘—π‘“β„“(π‘₯)

i.e. π€πœ“(π‘₯) =π€πœ‘(𝑓(π‘₯))𝐃𝑓(π‘₯) and thus

∣detπ΄πœ“(π‘₯)∣=|detπ΄πœ‘(𝑓(π‘₯))||det𝐃𝑓|

as required.

For 𝑔 ∈𝐺 we define the chart

πœ‘π‘”:π‘”π‘ˆβ†’πœ‘π‘”(π‘ˆ)β„Žβ†¦πœ‘(π‘”βˆ’1β„Ž)

then

βˆ’π‘–πœ‘βˆ’1𝑔(π‘₯)βˆ’1πœ•π‘—πœ‘βˆ’1𝑔(π‘₯)=βˆ’π‘–(π‘”πœ‘βˆ’1(π‘₯))βˆ’1π‘”πœ•π‘—πœ‘βˆ’1(π‘₯)=βˆ’π‘–πœ‘βˆ’1(π‘₯)βˆ’1πœ•π‘—πœ‘βˆ’1(π‘₯)

which gives left-invariance.

For each 𝑔 ∈𝐺 let π‘€π‘˜β„“(𝑔) so that π‘”βˆ’1π‘‹π‘˜π‘” =π‘‹β„“Ξ”β„“π‘˜(𝑔). Letting πœ“(β„Ž) =πœ“(β„Žπ‘”βˆ’1), i.e. πœ“βˆ’1(π‘₯) =πœ‘βˆ’1(π‘₯)𝑔, then

βˆ’π‘–πœ“βˆ’1(π‘₯)βˆ’1πœ•π‘—πœ“βˆ’1(π‘₯)=βˆ’π‘–π‘”βˆ’1πœ‘βˆ’1(π‘₯)βˆ’1πœ•π‘—πœ‘βˆ’1(π‘₯)𝑔=π‘›βˆ‘π‘˜=1π‘”βˆ’1π‘‹π‘˜π‘”π΄πœ‘π‘˜π‘—(π‘₯)=π‘›βˆ‘π‘˜,β„“=1π‘‹β„“π‘€β„“π‘˜(𝑔)π΄πœ‘π‘˜π‘—(π‘₯)

i.e. π΄πœ“ =𝑀(𝑔)π΄πœ‘. But

βˆ«πΊπ‘‘πœ‡(𝑔)=βˆ«πΊπ‘‘πœ‡(π‘”β€²β„Žβˆ’1)=∣det𝑀(β„Žβˆ’1)βˆ£βˆ«πΊπ‘‘πœ‡(𝑔)

and since 𝐺 is compact all integrals are finite, thus the ∣det𝑀(β„Žβˆ’1)∣ =1, i.e. 𝐺 is unimodular. Therefore πœ‡ is right-invariant.

Proof of uniqueness

Let πœ‡,𝜈 both be two sided Haar measures normalised such that πœ‡(𝐺) =𝜈(𝐺) =1. Then for any 𝑓 βˆˆβ„‚[𝐺]

βˆ«πΊπ‘“(𝑔)π‘‘πœ‡(𝑔)=βˆ«πΊβˆ«πΊπ‘“(𝑔)π‘‘πœ‡(𝑔)π‘‘πœˆ(β„Ž)=βˆ«πΊβˆ«πΊπ‘“(β„Žπ‘”)π‘‘πœ‡(𝑔)π‘‘πœˆ(β„Ž)=βˆ«πΊβˆ«πΊπ‘“(β„Ž)π‘‘πœ‡(𝑔)π‘‘πœˆ(β„Ž)=βˆ«πΊπ‘“(β„Ž)π‘‘πœˆ(β„Ž)

thus πœ‡ =𝜈.

Properties

Properties under integration

Let 𝑓 βˆˆβ„‚[𝐺] and πœ™ :𝐺 →𝐺 be a bijection (e.g. taking the inverse of each group element)

  1. βˆ«πΊπ‘“(β„Žπ‘”)π‘‘πœ‡(𝑔)=βˆ«πΊπ‘“(𝑔)π‘‘πœ‡(β„Žβˆ’1𝑔)=βˆ«πΊπ‘“(𝑔)π‘‘πœ‡(𝑔)
  2. βˆ«πΊπ‘“(π‘”β„Ž)π‘‘πœ‡(𝑔)=βˆ«πΊπ‘“(𝑔)π‘‘πœ‡(π‘”β„Žβˆ’1)=βˆ«πΊπ‘“(𝑔)π‘‘πœ‡(𝑔)
  3. βˆ«πΊπ‘“(πœ™(𝑔))π‘‘πœ‡(𝑔)=βˆ«πΊπ‘“(𝑔)π‘‘πœ‡(𝑔)
Proof of property 3

From properties 1 and 2

βˆ«πΊπ‘“(πœ™(𝑔))π‘‘πœ‡(𝑔)=βˆ«πΊπ‘“(β„Žπœ™(𝑔))π‘‘πœ‡(𝑔)=βˆ«πΊβˆ«πΊπ‘“(β„Žπœ™(𝑔))π‘‘πœ‡(β„Ž)π‘‘πœ‡(𝑔)=βˆ«πΊβˆ«πΊπ‘“(β„Ž)π‘‘πœ‡(β„Ž)π‘‘πœ‡(𝑔)=βˆ«πΊπ‘‘πœ‡(𝑔)

where we used the normalisation of the group to 1.


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Footnotes

  1. Here we use Keppeler's Lie algebra convention ↩