Sajet
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Hi! I have the following problem:
I tried to solve this by using the adjoint represantation and although it looks very promising, I can't really get it to work.
If I define [itex]C_x(y) := xyx^{-1}[/itex] as the conjugation, then what needs to be shown is: [itex]C_{h_1}h_2 = h_2[/itex].
I'm using these symbols: [itex]Ad: G \rightarrow GL(\mathfrak g), Ad(g) := C_{g*e}[/itex] and [itex]ad_X Y = [X, Y][/itex].
My idea is as follows: [itex][\mathfrak h_1, \mathfrak h_2] = 0[/itex] implies [itex]ad_{h_1}ad_{h_2}=ad_{h_2}ad_{h_1} \Rightarrow Ad_{*e}(h_1)Ad_{*e}(h_2) = Ad_{*e}(h_2)Ad_{*e}(h_1) \Rightarrow (Ad(h_1)Ad(h_2))_{*e} = (Ad(h_2)Ad(h_1))_{*e}[/itex]
[itex]\Rightarrow (Ad(h_1h_2))_{*e} = (Ad(h_2h_1))_{*e}[/itex]. Since [itex]G[/itex] is connected this implies [itex]Ad(h_1h_2) = Ad(h_2h_1) \Rightarrow C_{h_1h_2*e} = C_{h_2h_1*e} \Rightarrow C_{h_1h_2}= C_{h_2h_1} \Leftrightarrow C_{h_1} = C_{h_2h_1h_2^{-1}}[/itex] but I'm not getting any further from here.
Maybe this is the wrong path altogether but I don't see how else I could use the connectedness of G as well as the information on the Lie bracket to make a statement on the group elements themselves.
Let G be a connected Lie Group, [itex]\mathfrak g[/itex] its Lie algebra. Let [itex]\mathfrak h_1, \mathfrak h_2 \subset \mathfrak g[/itex] be subalgebras of [itex]\mathfrak g[/itex] with [itex][\mathfrak h_1, \mathfrak h_2] = 0[/itex], [itex]H_1, H_2[/itex] the subgroups belonging to them. Show: [itex]h_1h_2 = h_2h_1[/itex] for all [itex]h_1 \in H_1, h_2 \in H_2[/itex].
I tried to solve this by using the adjoint represantation and although it looks very promising, I can't really get it to work.
If I define [itex]C_x(y) := xyx^{-1}[/itex] as the conjugation, then what needs to be shown is: [itex]C_{h_1}h_2 = h_2[/itex].
I'm using these symbols: [itex]Ad: G \rightarrow GL(\mathfrak g), Ad(g) := C_{g*e}[/itex] and [itex]ad_X Y = [X, Y][/itex].
My idea is as follows: [itex][\mathfrak h_1, \mathfrak h_2] = 0[/itex] implies [itex]ad_{h_1}ad_{h_2}=ad_{h_2}ad_{h_1} \Rightarrow Ad_{*e}(h_1)Ad_{*e}(h_2) = Ad_{*e}(h_2)Ad_{*e}(h_1) \Rightarrow (Ad(h_1)Ad(h_2))_{*e} = (Ad(h_2)Ad(h_1))_{*e}[/itex]
[itex]\Rightarrow (Ad(h_1h_2))_{*e} = (Ad(h_2h_1))_{*e}[/itex]. Since [itex]G[/itex] is connected this implies [itex]Ad(h_1h_2) = Ad(h_2h_1) \Rightarrow C_{h_1h_2*e} = C_{h_2h_1*e} \Rightarrow C_{h_1h_2}= C_{h_2h_1} \Leftrightarrow C_{h_1} = C_{h_2h_1h_2^{-1}}[/itex] but I'm not getting any further from here.
Maybe this is the wrong path altogether but I don't see how else I could use the connectedness of G as well as the information on the Lie bracket to make a statement on the group elements themselves.