250 Boolean Analysis — Rotation
250.1 Overview
Gaussian rotations preserve the joint Gaussian law. Their disagreement probabilities satisfy continuity, subadditivity, and equal-step lower bounds.
250.2 Declarations
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). For any real \(t\), the map \((g,h)\mapsto (\cos t\, g+\sin t\, h,-\sin t\, g+\cos t\, h)\) preserves \(\gamma _n\otimes \gamma _n\).
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). Write \(s_A(t)\) for the real value of the product-measure mass \((\gamma _n\otimes \gamma _n)\{ (g,h):\mathbf1_A(g)\ne \mathbf1_A(\cos t\, g+\sin t\, h)\} \). If \(A\subseteq \mathbb R^n\) is measurable, then \(s_A(s+t)\le s_A(s)+s_A(t)\) for all real \(s,t\).
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). Write \(s_A(t)\) for the real value of the product-measure mass \((\gamma _n\otimes \gamma _n)\{ (g,h):\mathbf1_A(g)\ne \mathbf1_A(\cos t\, g+\sin t\, h)\} \). For any measurable \(A\subseteq \mathbb R^n\), integer \(\ell \ge 0\), and real angles \(\delta _1,\ldots ,\delta _\ell \), \(s_A(\sum _{j=1}^\ell \delta _j)\le \sum _{j=1}^\ell s_A(\delta _j)\).
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). Write \(s_A(t)\) for the real value of the product-measure mass \((\gamma _n\otimes \gamma _n)\{ (g,h):\mathbf1_A(g)\ne \mathbf1_A(\cos t\, g+\sin t\, h)\} \). For any measurable \(A\subseteq \mathbb R^n\), real \(\delta \), and positive integer \(\ell \), \(s_A(\delta )\le \ell \, s_A(\delta /\ell )\).
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). Write \(s_A(t)\) for the real value of the product-measure mass \((\gamma _n\otimes \gamma _n)\{ (g,h):\mathbf1_A(g)\ne \mathbf1_A(\cos t\, g+\sin t\, h)\} \). If \(A\subseteq \mathbb R^n\) is measurable and \(\alpha =\gamma _n(A)\), then \(s_A(\pi /2)=2\alpha (1-\alpha )\).
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). Write \(s_A(t)\) for the real value of the product-measure mass \((\gamma _n\otimes \gamma _n)\{ (g,h):\mathbf1_A(g)\ne \mathbf1_A(\cos t\, g+\sin t\, h)\} \). If \(A\subseteq \mathbb R^n\) is measurable with \(\gamma _n(A)=1/2\), then \(s_A(\pi /(2\ell ))\ge 1/(2\ell )\) for every positive integer \(\ell \).
Let \(n\ge 0\), let \(\gamma _n\) be standard Gaussian measure on \(\mathbb R^n\), and let \(G,G\prime \) be independent vectors with law \(\gamma _n\). Write \(s_A(t)\) for the real value of the product-measure mass \((\gamma _n\otimes \gamma _n)\{ (g,h):\mathbf1_A(g)\ne \mathbf1_A(\cos t\, g+\sin t\, h)\} \). For any measurable \(A\subseteq \mathbb R^n\), \(s_A(t)\to 0\) as the real angle \(t\to 0\).