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The $a_0^0(980)-f_0(980)$ mixing is one of the most potential tools to learnabout the nature of $a_0^0(980)$ and $f_0(980)$. Using the$f_0(980)$-$a_0^0(980)$ mixing intensity $\xi_{af}$ measured recently atBESIII, we calculate the the branching ratio of the the isospin violation decay$J/\psi \rightarrow\gamma\eta_c \rightarrow \gamma \pi^0 a_0^0(1450)\rightarrow\gamma \pi^0 a_0^0(980)f_0(500)\rightarrow \gamma \pi^0 f_0(980) f_0(500)\rightarrow \gamma \pi^0 \pi^+\pi^- \pi^+\pi^-$. The value of the branchingratio is found to be $O(10^{-6})$, which can be observed with $10^{10}$$J/\psi$ events collected at BESIII. The narrow peak from the$f_0(980)$-$a_0^0(980)$ mixing in the $\pi^+\pi^-$ mass square spectrum canalso be observed. In addition, we study the non-resonant decay$a_0^0(1450)\rightarrow f_0(980) \pi^+\pi^-(\text{non-resonant})$, which isdominated by the $a_0^0(980)$-$f_{0}(980)$ mixing. We find that thenon-resonant decay $a_0^0(1450)\rightarrow f_0(980) \pi^+\pi^-$ and the decay$a_0^0(1450)\rightarrow f_0(980) f_0(500)$ can be combined to measure themixing intensity $\xi_{af}$ in experiment. These decays are the perfectcomplement to the decay $\chi_{c1}\rightarrowf_{0}(980)\pi^{0}\to\pi^{+}\pi^{-}\pi^{0}$ which had been observed at BESIII,the observations of them will make the measurement of the mixing intensity$\xi_{af}$ more precisely.

Study of $a_0^0(980)$-$f_0(980)$ mixing from $a_0(1450) \to a_0^0(980) f_0(500) \to \pi^+ \pi^- f_0(500)$