Table 2 Critical disorder strength \(w_c\) and exponents \(\nu\), \(\zeta\) for different initial conditions (\(\theta ,\phi\)) for the quantities, square of total angular momentum operator \(\left\langle J^2 \right\rangle\) and von Neumann entropy \(S_{N/2}\) at \(k=1\), \(p=\pi /2\).
From: Chaos controlled and disorder driven phase transitions induced by breaking permutation symmetry
Quantity | \(w_c\) | \(\nu\) | \(\zeta\) |
|---|---|---|---|
\(J^2\) \((\theta =2.25\), \(\phi =1.1)\) | \(2.11 \pm 0.06\) | \(0.52 \pm 0.06\) | \(0.57 \pm 0.09\) |
\(J^2 (\theta =\pi /2,\phi =-0.56)\) | \(2.31 \pm 0.05\) | \(0.56 \pm 0.03\) | \(0.61 \pm 0.02\) |
\(J^2 (\theta =\pi /2, \phi =1.9)\) | \(1.1 \pm 0.09\) | \(0.54 \pm 0.01\) | \(0.64 \pm 0.06\) |
\(S_{N/2} (\theta =2.25, \phi =1.1)\) | \(1.93 \pm 0.06\) | \(0.60 \pm 0.06\) | \(0.68 \pm 0.07\) |
