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  "body": "\n## Definition\n\nThere is an absolute constant $c \u003e 0$ with the following property.\nLet $q \\ge 3$ be an integer and $\\chi$ a [[Dirichlet character|7XB5VJKDPG]] modulo $q$.\nThen the [[Dirichlet L-function|9D2Z543EJQ]] $L(s, \\chi)$ has no zero $s = \\sigma + it$ in the region\n$$\\sigma \\ge 1 - \\frac{c}{\\log\\big(q(\\abs{t} + 2)\\big)}.$$\nThe one possible exception is a single zero when $\\chi$ is a real nonprincipal character; such a zero is real and simple.\nFix such a constant $c$.\nA *Siegel zero* (or *exceptional zero*) for the modulus $q$ is a real number $\\beta$ with\n$$1 - \\frac{c}{\\log q} \u003c \\beta \u003c 1 \\quad\\text{and}\\quad L(\\beta, \\chi) = 0$$\nfor some real nonprincipal character $\\chi$ modulo $q$.\n\n## Remarks\n\nNo Siegel zero is known, so there is no example to check.\nIf the [[generalized Riemann hypothesis|DNKA4WBKDS]] holds, every zero of $L(s, \\chi)$ in the strip $0 \u003c \\operatorname{Re} s \u003c 1$ has real part $1/2$, so for large $q$ no Siegel zero exists.\nA non-example: a zero of $L(s, \\chi)$ for a character $\\chi$ that is not real is never a Siegel zero, because the zero-free region has no exception for such $\\chi$.\nSiegel's theorem bounds a possible exceptional zero: for every $\\varepsilon \u003e 0$ there is $c(\\varepsilon) \u003e 0$ with $\\beta \u003c 1 - c(\\varepsilon) q^{-\\varepsilon}$, but $c(\\varepsilon)$ is not effectively computable.\nThe notion depends on the choice of $c$; statements about Siegel zeros are usually about a sequence of moduli $q$ with $(1 - \\beta)\\log q \\to 0$.\n",
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