The joint distribution of every second eigenvalue obtained after superposing the spectra of two circular orthogonal ensembles ($\beta=1$) is known to be equal to that of the circular unitary ensemble… Click to show full abstract
The joint distribution of every second eigenvalue obtained after superposing the spectra of two circular orthogonal ensembles ($\beta=1$) is known to be equal to that of the circular unitary ensemble ($\beta=2$), where the parameter $\beta$ is the Dyson index of the ensemble. Superposition of spectra of $m$ such circular orthogonal ensembles is studied numerically using higher-order spacing ratios. It is conjectured that the joint probability distribution of every $k=m-2$-th $(m\geq4)$ eigenvalue corresponds to that of circular $\beta$-ensemble with $\beta=m-3$. For the special case of $m=3$, $k=\beta=3$. It is also conjectured that the spectral fluctuations corresponding to $k=m+1$ ($m\geq2$) and $k=m-3$-th ($m\geq5$) order spacing ratio distribution is identical to that of nearest neighbor spacing ratio distribution with Dyson indices $m+2$ and $m-4$ respectively. Strong numerical evidence in support of these conjectures is presented.
               
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