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The Arithmetic of Quaternion Algebra

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24 CHAPTER 2. QUATERNION ALGEBRA OVER A LOCAL FIELD<br />

otherwise. We call ε(H) the Hasse invariant <strong>of</strong> H.<br />

A variant <strong>of</strong> the above theorem is :<br />

Quat(K) � {∓1}, if K �= C, Quat(C) � {1}.<br />

Definition 2.2. If the characteristic <strong>of</strong> K is different from 2, and if a, b ∈ K × ,<br />

the Hasse invariant <strong>of</strong> a, b is defined by<br />

ε(a, b) = ε({a, b}),<br />

where H = {a, b} is the quaternion algebra described in Ch.I.(3). <strong>The</strong> Hilbert symbol<br />

<strong>of</strong> a, b is defined by<br />

�<br />

1, if ax<br />

(a.b) =<br />

2 + by2 − z2 = 0 has a non-trivial solution in K3 ,<br />

, −1, otherwise<br />

where the ”non-trivial solution” means a solution (x, y, z) �= (0, 0, 0).<br />

A variant <strong>of</strong> the above theorem in characteristic different from 2 is expressed<br />

as an equality between the Hilbert symbol and the Hasse invariant, and a variety<br />

<strong>of</strong> properties <strong>of</strong> Hilbert symbol deduced from it.<br />

Corollary 2.1.2. (Properties <strong>of</strong> Hilbert symbol). Let K is a local field <strong>of</strong> char.<br />

different from 2.Let a, b, c, x, y ∈ K × . <strong>The</strong> Hilbert symbol {a, b} equals the Hasse<br />

invariant ε(a, b). It satisfies the following properties:<br />

(1) (ax 2 , by 2 ) = (a, b) (modulo the square),<br />

(2) (a, b)(a, c) = (a, bc) (bilinearity),<br />

(3) (a, b) = (b, a)(symmetry),<br />

(4)(a,1-a) = 1 (symbol),<br />

(5) (a, b) = 1 for all b ∈ K × implies a ∈ K ×2 (non degenerate),<br />

(6)(a, b) = 1 is equivalent to one <strong>of</strong> the following properties:<br />

−a ∈ n(K( √ b))<br />

or b ∈ n(K( √ a)),<br />

or −ax 2 + by 2 represents 1<br />

Pro<strong>of</strong>. <strong>The</strong> equation ax 2 + by 2 − z 2 = 0 has a non trivial solution in H 3 if<br />

and only if the quadratic vector space V0 associated with pure quaternion <strong>of</strong><br />

{a, b} is isotropic. From ch.I, corollary 3.2, the space V0 is isotropic if and only<br />

if {a, b}is isomorphic to a matrix algebra. <strong>The</strong>refore (a, b) = 1 if and only if<br />

ε(a, b) = 1. it follows (a, b) = ε(a, b). <strong>The</strong> properties (1),(2),(3),(4),(5),(6) are<br />

the consequence <strong>of</strong> the earlier results.<br />

(1),(3): Define the elements i, j by the formula I.1.(3) and replace i, j by xi, yj,<br />

then by j, i.<br />

(2). Use the tensor product(I,Thm 2.9).<br />

(4),(6). Use the characterization <strong>of</strong> the matrix algebra (I,Corollary 2.4) and the<br />

geometric consideration (I,Corollary 3.2)<br />

(5).Obtain from that, all the quadratic extension <strong>of</strong> K can be included in the<br />

quaternion field over K, if K �= C. This property will be proved more precisely<br />

later(II,Corollary 1.9).<br />

We suppose afterwards that K �= R, C. <strong>The</strong> theorem <strong>of</strong> classification has the<br />

following very precise statement.

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