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The Arithmetic of Quaternion Algebra

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10 CHAPTER 1. QUATERNION ALGEBRA OVER A FIELD<br />

We now show the rotation (r, 2α) <strong>of</strong> the space R (identifying with the Hamilton<br />

quaternion <strong>of</strong> zero reduced trace) <strong>of</strong> angle 2α, and <strong>of</strong> the axis being carried out<br />

by a vector <strong>of</strong> r units, is induced by the inner automorphism associated with<br />

q = cos α + r sin α. In fact, we have r 2 = −1, and by the theorem 2.1 <strong>of</strong> automorphisms<br />

we can choose a quaternion s ∈ H such that s 2 = −1 and rs = −sr.<br />

<strong>The</strong> pure quaternions form the R-vector space with basis r, s, rs. Under this<br />

basis we shall verify the restriction <strong>of</strong> the inner automorphism induced by q to<br />

the quaternions with zero trace is the rotation defined above. We have:<br />

(cos α + r sin α)r(cos α − rsinα) = r,<br />

(cos α + r sin α)s(cos α − r sin α) = cos 2α.s + sin 2α.rs,<br />

(cos α + r sin α)s(cos α − r sin α) = cos 2α.rs − sin 2α.s.<br />

We derive from this that H 1 /∓1 is isomorphic to SO(3, R). We now show H 1<br />

is a non-trivial covering <strong>of</strong> SO(3, R). Otherwise, H 1 would contain a subgroup<br />

<strong>of</strong> index 2, hence distinguished. <strong>The</strong>re would exist a surjective homomorphism<br />

c <strong>of</strong> H 1 to ∓1. We shall see it is impossible. Since −1 is a square in H 1 , we<br />

have c(−1) = 1. All <strong>of</strong> the elements <strong>of</strong> square −1 being conjugated by an inner<br />

automorphism <strong>of</strong> H 1 , we have c(i) − c(j) = c(ij) or i, j are defined as that in<br />

§1. From it we obtain c(i) = 1, and c(x) = 1 for every quaternion <strong>of</strong> square −1.<br />

Because every quaternion <strong>of</strong> H 1 is the product <strong>of</strong> two quaternions <strong>of</strong> square<br />

−1 and <strong>of</strong> a sign, we then deduce c equals 1 on H 1 identically. We note that<br />

H 1 /∓1 being isomorphic to SO(3, R) is a simple group. It is well-known that<br />

P SL(2, K) = SL(2K)/∓1 is a simple group if the field K is not a finite field<br />

consisting <strong>of</strong> 2 or 3 elements (Dieudonné,[1]). the property can not be generalized.<br />

<strong>The</strong> group H 1 /∓1 is not always simple. It can be found in Dieudonné an<br />

infinite number <strong>of</strong> examples where the groups are not simple. Put the following<br />

question: if K is a global field, and H/K a quaternion algebra such that for the<br />

completion <strong>of</strong> Kv <strong>of</strong> K, the group Hv/∓1 is simple( where Hv = H ⊗ Kv), is<br />

Hv/∓1 a simple group? <strong>The</strong> group <strong>of</strong> commutator <strong>of</strong> a group G is the group<br />

generated by the elements <strong>of</strong> G <strong>of</strong> the form uvu −1 v −1 , u, v ∈ G. <strong>The</strong> group <strong>of</strong><br />

commutator <strong>of</strong> H × is then contained in H 1<br />

Proposition 1.3.5. <strong>The</strong> group <strong>of</strong> the commutators <strong>of</strong> H × equals H 1 .<br />

Pro<strong>of</strong>. Let h be a quaternion <strong>of</strong> reduced norm 1. If the algebra K(h) is a<br />

separable quadratic algebra over K, the theorem 90 <strong>of</strong> Hilbert indicates there<br />

exists an element x ∈ K(h) × such that h = xx −1 . We can moreover verify this<br />

property directly: if K(h) is a field, we choose x = h+1 if h �= −1, and x ∈ H × 0 ;<br />

if K(h) is not a field, it is isomorphic to K + K, and if h = (a, b) ∈ K + K is <strong>of</strong><br />

norm ab = 1, we then choose x = (c, d) with cd −1 = a. Since x, x are conjugate<br />

by an inner automorphism (they satisfy the same minimal polynomial), we<br />

deduce from this that h is a commutator.<br />

If K(h)/K is not separable quadratic extension, we then have h = h,hence (h −<br />

1) 2 = 0. If H is a field, then h = 1, otherwise H is isomorphic to M(2, K), and<br />

we would have the assertion: SL(2K) is the group <strong>of</strong> commutator <strong>of</strong> GL(2, K),<br />

cf. Dieudonneé[1].<br />

<strong>The</strong> explanation <strong>of</strong> the group H 1 /∓1 as the group <strong>of</strong> rotations <strong>of</strong> R 3 permits<br />

us to determine the structure <strong>of</strong> the finite groups <strong>of</strong> real quaternions as that <strong>of</strong><br />

finite rotation groups(Coxeter,[1]).We start from recalling this well-known result<br />

about the structure <strong>of</strong> finite rotation groups.

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