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For $ninmathbb N$ let $Theta^{(n)}$ be a random vector uniformly distributed on the unit sphere $mathbb S^{n-1}$, and consider the associated random probability measure $mu_{Theta^{(n)}}$ given by setting [ mu_{Theta^{(n)}}(A) := mathbb{P} left[ langle U, Theta^{(n)} rangle in A right],qquad U sim text{Unif}([-1,1]^n) ] for Borel subets $A$ of $mathbb{R}$. It is known that the sequence of random probability measures $mu_{Theta^{(n)}}$ converges weakly to the centered Gaussian distribution with variance $1/3$. We prove a large deviation principle for the sequence $mu_{Theta^{(n)}}$ with speed $n$ and explicit good rate rate function given by $I( u(alpha)) := - frac{1}{2} log ( 1 - ||alpha||_2^2)$ whenever $ u(alpha)$ is the law of a random variable of the form begin{align*} sqrt{1 - ||alpha||_2^2 } frac{Z}{sqrt 3} + sum_{ k = 1}^infty alpha_k U_k, end{align*} where $Z$ is standard Gaussian independent of $U_1,U_2,ldots$ which are i.i.d. $text{Unif}[-1,1]$, and $alpha_1 geq alpha_2 geq ldots $ is a non-increasing sequence of non-negative reals with $||alpha||_2<1$. We obtain a similar result for projections of the uniform distribution on the discrete cube ${-1,+1}^n$.
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Understanding transport processes in complex nanoscale systems, like ionic conductivities in nanofluidic devices or heat conduction in low dimensional solids, poses the problem of examining fluctuations of currents within nonequilibrium steady states