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Student Seminar: Classical and Quantum Integrable Systems

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is a representation of the group SU(2). Here<br />

g =<br />

( ) α β<br />

γ δ<br />

with α = ¯δ <strong>and</strong> γ = − ¯β is a group element of SU(2).<br />

Exercise 8<br />

Prove that<br />

⎛<br />

1 + c<br />

2<br />

2 1t 2 c 1 c 2 t 2 − c 3 t c 1 c 3 t 2 ⎞<br />

+ c 2 t<br />

α(φ) = −I + ⎝ c<br />

1 + c 2 t 2 2 c 1 t 2 + c 3 t 1 + c 2 2t 2 c 2 c 3 t 2 − c 1 t ⎠<br />

c 3 c 1 t 2 − c 2 t c 3 c 2 t 2 + c 1 t 1 + c 2 3t 2<br />

is a one-parameter subgroup in SO(3), where tan φ 2 = ct, c2 = c 2 1 + c 2 2 + c 2 3 <strong>and</strong><br />

⃗c = (c 1 , c 2 , c 3 ) is a constant vector.<br />

Exercise 9<br />

Let<br />

⎛<br />

cos ϕ − sin ϕ<br />

⎞<br />

0<br />

⎛<br />

1 0<br />

⎞<br />

0<br />

B ϕ = ⎝ sin ϕ cos ϕ 0 ⎠ , C θ = ⎝ 0 cos θ − sin θ ⎠ .<br />

0 0 1<br />

0 sin θ cos θ<br />

Show that any matrix A ∈ SO(3) can be represented in the form<br />

A = B ϕ C θ B ψ .<br />

Write the one-parameter subgroup from the exercise 8 in the coordinates (ϕ, θ, ψ).<br />

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