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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).

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