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Let \(E_r(n,t):=q_{\mathrm{sm}}^{4t}+q_{\mathrm{big}}^{4t}+e^{-a_r t n^{-2/3}}\). Then for every \(\delta \in (0,\pi /4)\),
Both are \(o(\hat A_{n,4t})\) as \(n\to \infty \) with \(t/(n^{8/3}\log t)\to \infty \).
Let \(\psi _G\) be the characteristic function obtained by replacing the Rademacher entries \(\xi _i\) with i.i.d. standard Gaussians \(g_i\). For each row \(k\in [n]\), define the row influence \(I_k(\lambda ):=\sum _{i\ne k}\lambda _{\{ i,k\} }^2\), and set \(J(\lambda ):=\sum _{k=1}^n I_k(\lambda )^{3/2}\). Then
The formalization proves the following (as private lemmas in HadamardCn3TorusCount.lean):
Multiplicativity: \(\psi (\lambda +\gamma )=\psi (\lambda )\psi (\gamma )\) for \(\lambda \in \Lambda \), \(\gamma \in \mathcal{B}_{\pi /4}\) (psi_translate_lambdaReal).
Disjoint boxes: the translates \(\mathcal{B}_\delta (\lambda )\), \(\lambda \in \Lambda \), are pairwise disjoint for \(\delta {\lt}\pi /4\) (translated_edgeBoxes_disjoint).
Cardinality: \(|\Lambda |=2^{2d-n+1}\) and \(\psi (\lambda )^{4t}=1\) for \(\lambda \in \Lambda \) (card_lambdaShifts_eq_pow_of_two_le, exp_phase_lambdaReal_false_pow_four_mul).
Even-degree characterization: \(\lambda \in \Lambda \) iff every vertex of \(G_{\lambda ^{(2)}}\) has even degree (parityEvenBool_iff_incidence_zero).
These are private because they are only used internally by the torus counting machinery.
Let \(A\) be a complex symmetric \(m\times m\) matrix whose real part is positive definite. Then \(\int _{\mathbb {R}^m}e^{-x^\top A x}\, dx=\pi ^{m/2}\det (A)^{-1/2}\). In particular, if \(g\sim N(0,I_m)\) and \(M\) is real symmetric, \(|\mathbb {E}[e^{ig^\top Mg/2}]|=\det (I+M^2)^{-1/4}\).
Let \(A\) be a symmetric zero-diagonal \(n\times n\) matrix, \(B\) the \((n{-}1)\times (n{-}1)\) submatrix deleting row/column \(n\), \(x\in \mathbb {R}^{n-1}\) the last column, and \(M(B)=B^2-\operatorname {diag}(B^2)\). Then
For \(0{\lt}\delta {\lt}\pi /4\),
and the sets in the union are disjoint.
Let \(f:[n]^2\to \mathbb {R}\) be symmetric with \(f(i,i)=0\), and define
If \(X_1,\dots ,X_n\) are independent Rademacher signs, \(G_1,\dots ,G_n\) are i.i.d. \(N(0,1)\), and \(\varphi :\mathbb {R}\to \mathbb {R}\) is \(C^3\), then
Set \(\eta _r:=\frac{1}{3}[1-(1+2r^2)^{-1/4}]\) and \(I_{\max }(\lambda ):=\max _k I_k(\lambda )\). There exist \(q_{\mathrm{sm}},q_{\mathrm{big}}\in (0,1)\) and \(a_r{\gt}0\) such that for all \(n\ge 2\) and \(t\ge 1\) the far shell decomposes as
and
Set \(K_n:=2^{2d-n+1}(2\pi )^{-d}\). For all sufficiently large \(n\) and \(t\ge C_0 n^3\),
There exist \(c_1,C_1{\gt}0\) such that if \(d/t\le c_1\) and \(nd^2/t^2\le c_1\), then
and
Set \(\delta ^2=2d/t\) and \(K_n:=2^{2d-n+1}(2\pi )^{-d}\). Then
as \(n\to \infty \) with \(t/(n^{8/3}\log t)\to \infty \). For \(t\ge C_0 n^3\) and all sufficiently large \(n\), both bounds are at most \(Ce^{-cn^2}\hat A_{n,4t}\).