John Stillwell - Naive Lie Theory.pdf - Index of
John Stillwell - Naive Lie Theory.pdf - Index of
John Stillwell - Naive Lie Theory.pdf - Index of
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56 3 Generalized rotation groups<br />
Path-connectedness <strong>of</strong> SU(n)<br />
We can prove that SU(n) is path-connected, along similar lines to the pro<strong>of</strong><br />
for SO(n) in the previous section. The pro<strong>of</strong> is again by induction on n,<br />
but the case n = 2 now demands a little more thought. It is helpful to use<br />
the complex exponential function e ix , which we take to equal cosx + isinx<br />
by definition ( for now. ) (In Chapter 4 we study exponentiation in depth.)<br />
α −β<br />
Given in SU(2), first note that (α,β) is a unit vector in C 2 ,<br />
β α<br />
so α = ucosθ and β = vsinθ for some u,v in C with |u| = |v| = 1. This<br />
means that u = e iφ and v = e iψ for some φ,ψ ∈ R.<br />
It follows that<br />
α(t)=e iφt cos θt, β(t)=e iψt sinθt, for 0 ≤ t ≤ 1,<br />
gives a continuous path<br />
SU(2) is path-connected.<br />
( α(t) −β(t)<br />
β(t) α(t)<br />
)<br />
from 1 to<br />
( α −β<br />
β α<br />
)<br />
in SU(2). Thus<br />
Exercises<br />
Actually, SU(2) is not the only special unitary group we have already met, though<br />
the other one is less interesting.<br />
3.3.1 What is SU(1)?<br />
The following exercises verify that a linear transformation <strong>of</strong> C n , with matrix<br />
A, preserves the Hermitian inner product (*) if and only if AA T = 1. They can be<br />
proved by imitating the corresponding steps <strong>of</strong> the pro<strong>of</strong> in Section 3.1.<br />
3.3.2 Show that vectors form an orthonormal basis <strong>of</strong> C n if and only if their<br />
conjugates form an orthonormal basis, where the conjugate <strong>of</strong> a vector<br />
(u 1 ,u 2 ,...,u n ) is the vector (u 1 ,u 2 ,...,u n ).<br />
3.3.3 Show that AA T = 1 if and only if the row vectors <strong>of</strong> A form an orthonormal<br />
basis <strong>of</strong> C n .<br />
3.3.4 Deduce from Exercises 3.3.2 and 3.3.3 that the column vectors <strong>of</strong> A form<br />
an orthonormal basis.<br />
3.3.5 Show that if A preserves the inner product (*) then the columns <strong>of</strong> A form<br />
an orthonormal basis.<br />
3.3.6 Show, conversely, that if the columns <strong>of</strong> A form an orthonormal basis, then<br />
A preserves the inner product (*).