The Arithmetic of Quaternion Algebra
The Arithmetic of Quaternion Algebra
The Arithmetic of Quaternion Algebra
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3.2. ZETA FUNCTION, TAMAGAWA NUMBER 55<br />
Pro<strong>of</strong>. When X is a field, the computation <strong>of</strong> Tamagawa number is implicitly<br />
contained in the theorem 2.2 <strong>of</strong> the functional equation. If X = M(2, K) , it<br />
can compute directly. <strong>The</strong> theorem 2.3 can be extended to the central simple<br />
algebra X. In this case we have τ(X) = τ(X1) = τ(H 1 ) = 1 and τ(G) = n,<br />
if [X : K] = n 2 . Reference: Weil [2]. By the definition <strong>of</strong> Tamagawa measure,<br />
τ(X) = 1. We shall prove τ(G) = 2τ(H 1 ) and τ(H1) = τ(H 1 ), after that then<br />
τ(H 1 ) = 1. <strong>The</strong> pro<strong>of</strong> is analytic, and the Poisson formula is involved. <strong>The</strong><br />
exact sequence which is compatible with thee Tamagawa measures<br />
1 −−−−→ H 1 A /H×<br />
K<br />
−−−−→ HA,1/H ×<br />
K<br />
n<br />
−−−−→ KA,1/K × −−−−→ 1<br />
proves that τ(H 1 ) = τ(H1)τ(K −1<br />
1 ). <strong>The</strong> theorem 2.2 shows τ(H1) = τ(K1) = 1<br />
if H is a field because <strong>of</strong> the definition <strong>of</strong> Tamagawa measure itself. <strong>The</strong>refore<br />
τ(H 1 = τ(H1) for every quaternion algebra H/K. It follows from the pro<strong>of</strong> <strong>of</strong><br />
<strong>The</strong>orem 2.2 that<br />
�<br />
2<br />
K ×<br />
A /K×<br />
H ×<br />
A /H×<br />
f(||h||H)dhA<br />
K<br />
·τ(H1 )<br />
f(||k||K)dk ∗ A =<br />
K ×<br />
A /K×<br />
�<br />
K ×<br />
A /K×<br />
f(||k|| K 2)dk ∗ A<br />
for every function f such that the integrals converge absolutely. Applying<br />
||h||H = ||n(h)|| K2 if h ∈ H times<br />
A , we see that<br />
�<br />
�<br />
f(||k||K)dk ∗ �<br />
A = τ(G)<br />
K ×<br />
A /K×<br />
f(||k||K)dkA∗, it follows τ(G) = 2τ(H 1 ). <strong>The</strong> <strong>The</strong>orem has been proved when X = H or K is<br />
a field.<br />
It remains to prove τ(SL(2, K)) = 1. <strong>The</strong> starting point is the formula<br />
�<br />
�<br />
(2) f(x)dx =<br />
[<br />
�<br />
f(ua)]τ(u),<br />
A 2<br />
SL(2,A)/SL(2,K)<br />
a∈K 2 −<br />
where f is an admissible function on A 2 , cf. II,§2, and τ(u) is a Tamagawa<br />
measure on SL(2, A)/SL(2, K), and where A 2 is identified with the column<br />
vectors <strong>of</strong> two elements in A on which SL(2, A) operates by<br />
� � � � � �<br />
a b x ax + by<br />
=<br />
.<br />
c d y cx + dy<br />
� �<br />
0<br />
<strong>The</strong> orbit <strong>of</strong> is A<br />
1<br />
2 � �<br />
� �<br />
0<br />
1 x<br />
− and its isotropic group is NA = { |x ∈ A}.<br />
0<br />
0 1<br />
We apply Poisson formula,<br />
�<br />
f(ua) = �<br />
f ∗ ( t u −1 a)<br />
a∈K 2<br />
a∈K 2<br />
because <strong>of</strong> det(u) = 1. Here we give an other expression for the integral (2) in<br />
function <strong>of</strong> f ∗ . In fact, it prefers to write the integral in f ∗ into the function on<br />
f ∗∗ = f(−x). Since τ( tu−1 ) = τ(u), we obtain<br />
(3)<br />
�<br />
A 2<br />
f ∗ �<br />
(x)dx =<br />
SL(2,A)/SL(2,K)<br />
a∈K2 ⎛<br />
⎝0 0<br />
⎞<br />
⎠<br />
[ �<br />
f(ux) − f ∗ (0)]τ(u).