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A great deal of early information can be found in the first edition of the Particle Data Book~\cite{Rosenfeld:1964xte} published in 1964, and the subsequent version~\cite{Rosenfeld:1965yz} published in 1965. 
\begin{itemize}
\item The $S(975)$ or the $S^{*}$ is now known as the $f_{0}(980)$. The $S^{*}$ was reported in 1966~\cite{Crennell:1966ry}. The state was first reported in the reaction $\pi^{+}p\rightarrow\Delta^{++}\pi^{+}\pi^{-}$ and $\pi^{+}p\rightarrow \Delta^{++} K^{+}K^{-}$ in 1973~\cite{Protopopescu:1973sh}. 

\item The $\delta(980)$ is now known as the $a_{0}(980)$. The state was first reported in $\bar{p}p\rightarrow K_{S}K^{\pm}\pi^{\mp}$ at rest, where the analysis focused on events without $K^{*}(890)$ in 1965~\cite{Armenteros:1965zz}.

\item The $H(1190)$ is now known as the $h_{1}(1170)$.  The state was first observed in $\pi^{-}p\rightarrow \pi^{+}\pi^{-}\pi^{0}n$ in 1981~\cite{Dankowych:1981ks}.

\item The $B(1235)$ is now known as the $b_{1}(1235)$. The state was first observed in an analysis of reactions of the type $\pi^{+}p\rightarrow p X$ in 1963.~\cite{Abolins:1963zz}

\item The $f(1270)$ is now known as the $f_{2}(1270)$. The state was first observed in $\pi^{-}p\rightarrow n\pi^{+}\pi^{-}$ in 1963~\cite{Bondar:1963zz}.

\item  The $A(1270)$ or the $A_{1}$ is now known as the $a_{1}(1260)$. An enhancement in the region of the $a_{1}$ mass was first observed in $\pi^{-}$ interactions on carbon. The authors separated their data into classes of events based on the number of pions. The so-called $A$
 region contained $\pi^{+}\pi^{-}\pi^{-}$ events and a broad enhancement was seen~\cite{Bellini:1963zz}. The $A$ name stuck for mesons in this mass region. In subsequent work~\cite{Goldhaber:1964zz,Chung:1964zza}, two states were resolved: the $A_{1}$ and $A_{2}$.
%The state was first observed in a collective analysis of both $\pi^{+}p$ and $\pi^{-}p$ reactions. It was first reported in 1975~\cite{Bowler:1975my}.

\item  The $D(1285)$ is now known as the $f_{1}(1285)$. The state was first reported in $\pi^{-}p$ interactions in three or more-body final states. It was first reported in 1967~\cite{Dahl:1967pg}

\item  The $\epsilon(1300)$ is know known as the $f_{0}(1370)$. The state was first reported in $\bar{p}n\rightarrow\pi^{+}\pi^{+}\pi^{-}\pi^{-}\pi^{-}$ annihilation at rest as an enhancement in $\rho\rho$. It was first reported in 1966~\cite{Bettini:1966zz}.

\item  The $A_{2}(1320)$ is now known as the $a_{2}(1320)$. This appears to be firest reported in $\pi p$ interactions, but I have been unable to track down the earliest reference. It was orignially discussed as part of the $A$ which ultimately included both the $A_{1}$ and $A_{2}$~\cite{Bellini:1963zz,Goldhaber:1964zz,Chung:1964zza}.

\item  The $E(1420)$ is now known as the $f_{1}(1420)$. The $E(1420)$ and the $\iota(1440)$ have a bit of a confused history. A state called the $E$ with $J^{PC}=0^{-+}$ was first reported in $\bar{p}p\rightarrow K\bar{K}3\pi$ in the $K\bar{K}\pi$ invarant mass~\cite{Baillon:1967zz}. The $E$ was first reproted oin   $J^{PC}=0^{-+}$ was reported in radiateive $J/\psi$ decays in $K\bar{K}\pi$~\cite{Scharre:1980zh}. A $J^{PC}=1^{++}$ state was later observed in $\pi p$ inetarcations~\cite{CERN-CollegedeFrance-Madrid-Stockholm:1980umk} and by 1984, the $E$ was assigned $J^{PC}=1^{++}$ quantum numbers and the $\iota$ was assigned $J^{PC}=0^{-+}$ quantum numbers. Hence, older literature will likely be very confused on these two states. The pseudoscalar states are prodcued strongly in both radaitive $J/\psi$ decays and proton antiproton annilation at rest. The axial state is produced in central production, photoproduction and $\pi p$ interactions. 

\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 $f_{2}^{\prime}(1525)$. This state was first observed in $K^{-}p$ unteractions in $_{S}K_{S}$ recoiling against a hyperon. The original observation is from 1965~\cite{Barnes:1965pc} and a spin parity analysis from 1966~\cite{Barnes:1967pe}.

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

\item  The $A(1680)$ or $A_{3}$ is now known as the $\pi_{2}(1670)$. The state was first observed in the reaction $\pi^{\pm} p \rightarrow p \pi^{\pm} \pi^{+} \pi^{-}$ in the three pion invariant mass~\cite{Bartsch:1968zz,Baltay:1968zza}. It was reported in a conference in 1966, but the first published observations were in 1968.

\item  The $\theta(1690)$ is now known as the $f_{0}(1710)$. There was early uncertainty whether it was $J^{PC}=0^{++}$ or $2^{++}$. It is now confirmed as $0^{++}$.The state was reported in $\pi^{-}p\rightarrow K_{S}K_{S}n$~\cite{Etkin:1981sg,Etkin:1982se}, where is was identified as $J^{PC}=0^{++}$ and called the $S^{*}$. In radiative $J/\psi$ decyas, $J/\psi\rightarrow \gamma\eta\eta$, a state identified as $J^{PC}=2^{++}$ and called the $\theta$~\cite{Edwards:1981ex} was reported. Finally, an enhancement below $2$~GeV was reported in $J/\psi\rightarrow\rho^{0}\rho^{0}$~\cite{Burke:1982am}. All of these observations were reported in 1982.

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

\item The $h(2030)$ is now known as the $f_{4}(2050)$. This state was observed in $\pi^{-} p \rightarrow n \pi^{0} \pi^{0}$ and reported as the $h$ meson~\cite{Serpukhov-CERN:1975qnq}. It was also reported in $\pi^{-} p \rightarrow n K^{+} K^{-}$ and also reportd as the $h$~\cite{CERN-MUNICH:1975yng}. Both of these observations are from 1975.

\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}
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