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4.4 Geometry of the special unitary

4.4.1 Special The special unitary group is the generalization of the special to the complex numbers. The group is defined as

SUn = {P ∈ Un | det(P ) = 1}.

Example 4.4.2. The case n = 1. This is a toy example. It is clear that SU1 is the set of complex numbers having length one, in other words SU1 is the 2 unit circle in the plane R . We have earlier identified the group SO2 with the circle, and therefore also that SO2 = SU1.

Lemma 4.4.3. Elements P ∈ SU2 are of the form a −b P = b a with any complex numbers a and b such that aa + bb = 1. We have a map 4 ϕ: SU2 −→ R , sending a to the vector determined by its first column. 2 2 3 2 4 The map identifies SU2 with the unit 3-sphere {x1 + x2 + x3 + x4 = 1} ⊂ R . In particular the 3-sphere has a group structure.

a c Proof. Let P = [ b d ] be an element of SU2. As det(P ) = 1 we have the two following expressions for the inverse of P , namely

 d −c a b P −1 = = P ∗ = . −b a c d

This gives us that d = a and that c = −b. In other words we have that

a −b P = , b a where det(P ) = aa + bb = 1. If we write out the complex numbers as

a = x1 + ix2 and b = x3 + ix4, then the map ϕ takes P to ϕ(P ) = (x1, x2, x3, x4). Then ϕ(P ) is a point on the unit 3-sphere. It is clear that the map ϕ is injective, and also surjective.

Remark 4.4.4. A remarkable result from topology shows that the 1-sphere and the 3-sphere are the only spheres that allow a group structure.

75  a −b  Lemma 4.4.5. Let P = b a be an element of SU2. Write a = x1 + ix2. Then, for any Q we have that characteristic polynomial of QP Q∗ is 2 t − 2x1t + 1. Moreover, the eigenvalues of QP Q∗ are complex conjugates λ and λ, only depending on the Trace(QP Q) = 2x1. In particular the matrix P is conjugate to the diagonal matrix λ 0 . 0 λ Proof. As Q is unitary we have that QQ∗ = 1. Therefore the characteristic polynomial cP (t) = det(t − P ) is invariant for conjugate matrices. Indeed, we have that

∗ ∗ ∗ cP (t) = det(Q) det(t − P ) det(Q ) = det(Q(t − P )Q ) = det(t − QP Q ), where the last expression is the characteristic polynomial of QP Q∗. As P is in SU2 is thas one, and a computation gives that

2 2 cP (t) = t − (a + a)t + 1 = t − 2x1 + 1.

p 2 The roots of the characteristic polynomial are x1 ± x1 − 1, hence the eigen- values are . Since a unitary matrices are normal we have that P is normal, and by Theorem 4.3.16 we have that P is conjugate to a diagonal matrix. A diagonal matrix must neccessarily have its eigenvalues on the diagonal.

Remark 4.4.6. Let P be an element of SU2. With the notation as in the p 2 above lemma we have that the eigenvalues of P are x1 ± x1 − 1. Thus the two eigenvalues λ and λ are distinct as long as x1 6= ±1. Then P is conjugate to two diagonal matrices obtained by changing the of its eigenvalues. By the lemma above we have that P must be conjugate to at least one of  λ 0  0 1 ∗ these, say D = 0 λ . The matrix Q = [ −1 0 ] is unitary, and such that QDQ is a diagonal but with λ interchanged with λ. In the cases when x1 = ± then there is only only diagonal matrix in the orbit, namely I and −I.

4.4.7 Latitudes The points (±1, 0, 0, 0) of the unit 3-sphere are identified as the north and south pole. The latitudes at −1 ≤ c ≤ 1 is then obtained as the intersection of the plane x1 = c and the unit 3-sphere. Thus, the latitude is given by

2 2 2 2 x2 + x3 + x4 = (1 − c ).

76 √ The latititudes are 2-spheres with radie ( 1 − c2) when c 6= ±1, and simply the poles when c = ±1.

Proposition 4.4.8. The conjugacy classes in SU2 are the latitudes of the unit 3-sphere. For a given −1 ≤ c ≤ 1 the corresponding latitude consists of all matrices P ∈ SU2 having trace Trace(P ) = 2c. In particular trace zero matrices form the equator. The two special latitudes c = ±1, i.e. the poles, consits each of one single element {I} and {−I}, and do together form the of the group SU2. Proof. The statements follows by Lemma 4.4.5.

4.4.9 Longitudes A longitude of the 3-sphere S we define as the intersection of S with a 2-dimensional plane passing through the poles. A longitude is then a 1- dimensional circle. There is a unique line passing through the two poles of the sphere S. Thus, if P is any point on the sphere, different from the poles, there will be a unique plane containing P and the poles, hence there is a unique longitude passing through P . 4 Let W ⊆ R be the plane x3 = x4 = 0. For any w = (w1, w2, 0, 0) ∈ W we let P =  w1+iw2 0 . Then the longitude W ∩ S are the matrices P w 0 w1−iw2 w such that det(Pw) = 1. Elements in this particular longitude are then the matrices λ 0 W ∩ S = { | λλ = 1}. 0 λ

4 Lemma 4.4.10. Let Q be an element of SU2. The map W −→ R sending 1 w 7→ QP Q∗ w 0 is an R-linear, injective map.

 a −b  Proof. Write Q = b a . We then compute that

a −b λ 0  a b aaλ + bbλ ab(λ − λ) QP Q∗ = = . b a 0 λ −b a ab(λ − λ) aaλ + bbλ

The map in question takes w ∈ W to the first column of the matrix QP Q∗. Write now a = x1 + ix2 and b = x3 + ix4. Then we obtain that

2 2 2 2 2 2 2 2 aaλ + bbλ = (x1 + x2 + x3 + x4)w1 + i(x1 + x2 − x3 − x4)w2.

77 And, for ab(λ − λ) we get the expression

2(x2x3 − x1x4)w2 + i2(x1x3 + x2x4)w2. Hence we have that the map is real linear. Infact, the matrix representation of this map in the standard basis is 1 0  0 x2 + x2 − x2 − x2 A =  1 2 3 4 . 0 2(x2x3 − x1x4)  0 2(x1x3 + x2x4) We need to see that the matrix A has two. Assume that coefficients 2 2 2 2 of the second column of A vanishes. Using that x1 + x2 + x3 + x4 = 1 2 − 2 4 2 2 1 2 2 together with x1 + x2 x3 − x2 = 0 gives that x1 + x2 = 2 = x3 + x4. Thus q 1 2 q 1 2 x2 = ± 2 − x1 and x3 = ± 2 − x4. Then the two remaining coeffcients 2 2 2 2 2 2 2 2 1 2 1 1 2 give x2x3 + x1x3 = x1x4 + x2x4. Which gives 2 x3 = 2 ( 2 − x3). The solutions 1 are then that all coordinates x1, x2, x3 and x4 are ± 2 . Then, by checking, one sees that one is not able to choose parities such that x2x3 = x1x4 and x1x3 = −x2x4 are satisfied simultaneously. Hence, we have that the matrix A has rank two.

Proposition 4.4.11. The longitudes of SU2 are the conjugate of T , that is subgroups of the form

∗ ∗ Q(W ∩ S)Q = {QDλQ | Dλ ∈ T }, with Q ∈ SU2. Proof. We need to show that QT Q∗ is a longitude for any given Q, and that every longitude is of this particular form. By Lemma 4.4.10 we have that ∗ 4 4 QT Q determines a real W −→ R . The VQ ⊆ R is a plane that contains the poles (±1, 0, 0, 0), and consquently VQ ∩ S is a longitude. ∗ By construction the longitude VQ ∩ S is the conjugate QT Q .A point P on the sphere corresponds to a matrix in SU2. By Lemma 4.4.5 the P is conjugate to a diagonal D matrix, hence of the form P = QDQ∗. Thus, all longitudes are conjugate subgroups QT Q∗. Exercises. Special unitary group. 1. Let x and y be two points on the unit 3-sphere S, which is a group. Compute the coordinates for the product x · y.

2. Show that the subgroup SO2 of SU2 is a longitude on the unit 3-sphere S.

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