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\begin{document}
\begin{itemize}
\item The $S(975)$ or the $S^{*}$ is now known as the $f_{0}(980)$.

\item The $\delta(980)$ is now known as the $a_{0}(980)$.

\item The $H(1190)$ is now known as the $h_{1}(1170)$.

\item The $B(1235)$ is now known as the $b_{1}(1235)$.

\item The $f(1270)$ is now known as the $f_{2}(1270)$.

\item  The $A(1270)$ or the $A_{1}$ is now known as the $a_{1}(1270)$.

\item  The $D(1285)$ is now known as the $f_{1}(1285)$.

\item  The $\epsilon(1300)$ is know known as the $f_{0}(1370)$.

\item  The $A_{2}(1320)$ is now known as the $a_{2}(1320)$.

\item  The $E(1420)$ is now known as the $f_{1}(1420)$.

\item  The $\iota(1440)$ is now two states, the $\eta(1405)$ and the $\eta(1475)$.

\item  The $f^{\prime}(1525)$ is now known as the $f_{2}^{\prime}(1525)$.

\item  The $\omega(1670)$ is now known as the $\omega_{3}(1670)$.

\item  The $A(1680)$ or $A_{3}$ is now known as the $\pi_{2}(1670)$.

\item  The $\theta(1690)$ is now known as the $f_{0}(1700)$. There was early uncertainty whether it was $J^{PC}=0^{++}$ or $2^{++}$. It is now confirmed as $0^{++}$.

\item The $\phi(1850)$ is now known as the $\phi_{3}(1850)$.

\item The $h(2030)$ is now known as the $f_{4}(2050)$.

\item The $Q(1280)$ or $Q_{1}$ is now known as the $K_{1}(1270)$.
  
\item The $\kappa(1350)$ is now known as the $K^{*}_{0}(1430)$.

\item The $Q(1400)$ or $Q_{2}$ is now known as the $K_{1}(1400)$.
  
\item The $K^{*}(1430)$ is now known as the $K^{*}_{2}(1430)$

\item The $L(1770)$ is now known as the $K_{2}(1770)$.

\item The $K^{*}(1780)$ or $K^{*}$ is now known as the $K^{*}_{3}(1780)$.

\item The $K^{*}(2060)$ is now known as the $K^{*}_{4}(2045)$.
  
\end{itemize}
\end{document}