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A PRIMER OF ANALYTIC NUMBER THEORY: From Pythagoras to ...

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13.3 Siegel Zeros and the Class Number 323<br />

every term in �(t, F). Then, (13.10) implies that<br />

�(s, F) ≥ 1 1<br />

−<br />

s − 1 s .<br />

When F(x, y) is the principal class, throw out everything except the summand<br />

(x, y) = (1, 0) in the first integral. Because F(1, 0) = 1, (13.10) implies that<br />

�(s, F) ≥ 1 1<br />

−<br />

s − 1 s +<br />

� ∞<br />

exp(−2�t/ � s dt<br />

|d|)t<br />

t<br />

1<br />

in this case. We now sum these inequalities over all h equivalence classes <strong>to</strong><br />

get<br />

�(s, d) ≥<br />

h<br />

s(s − 1) +<br />

� ∞<br />

1<br />

exp(−2�t/ � |d|)t<br />

s dt<br />

, (13.14)<br />

t<br />

where we used (13.9) <strong>to</strong> sum the expressions �(s, F) and where we put the h<br />

expressions 1/(s − 1) − 1/s over a common denomina<strong>to</strong>r. Now, (13.11) says<br />

that the left side above is<br />

�(s, d) = h<br />

+ O(1) as s → 1.<br />

s − 1<br />

So, particularly when s approaches 1 from below, the function is negative,<br />

because then 1/(s − 1) →−∞. The GRH would then say it must be negative<br />

for all s between 1/2 and 1; it cannot change signs. Otherwise, it is<br />

certainly negative for � < s < 1, where � is the rightmost counterexample<br />

<strong>to</strong> GRH. Now is a good time <strong>to</strong> point out that any possible counterexamples<br />

<strong>to</strong> GRH must come from L(s, �d) in the fac<strong>to</strong>rization (13.9). The term<br />

2|d| s/2 (2�) −sƔ(s) is positive for s > 0, and we proved in Section 8.1 that<br />

�(s) has no real zeros on the interval 0 < s < 1.<br />

Hecke’s idea was simply <strong>to</strong> investigate the consequences for (13.14) of the<br />

inequality �(s, d) < 0. We have<br />

0 >�(s, d) ≥<br />

h<br />

s(s − 1) +<br />

� ∞<br />

which, on rearranging the terms, says that<br />

� ∞<br />

h > s(1 − s) exp(−2�t/ � s dt<br />

|d|)t<br />

t .<br />

1<br />

1<br />

exp(−2�t/ � s dt<br />

|d|)t<br />

t ,<br />

If we integrate over an even smaller range, √ |d| ≤t, the integral is yet smaller,<br />

and we then change the variables in the integral with u = t/ √ |d|, which

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