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\Large{\bf A Second Look at Single Photon Production in $S+Au$ Collisions
 at 200 A$\cdot$GeV and Implications for Quark Hadron Phase Transition}
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\large{Dinesh Kumar Srivastava$^1$  and Bikash Chandra Sinha$^{1,2}$}
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\large{\em $^1$ Variable Energy Cyclotron Centre,\\
 1/AF Bidhan Nagar, Calcutta 700 064, India\\

$^2$ Saha Institute of Nuclear Physics,\\
1/AF Bidhan Nagar, Calcutta 700 064, India\\}

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\large{Erratum: Eur. Phy. J. C 12 (2000) 109.}
Abstract

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It has been recently shown~\cite{MT} that the values of $J_T$ and $J_L$
which appear in Eq.(2) and (5) are too large by a factor of 4,
in the Ref.~\cite{pat}. Correcting for this changes the Fig.~2 (see below).
More-over, now the emissions from the quark matter dominate only for
$p_T <$ 1 GeV/$c$. The basic result of the paper, that the
upper limit of the single-photon production is consistent with the
rates for photon production at two-loop level remains valid.

\bigskip
 
\begin{thebibliography}{37}

\bibitem{pat} P. Aurenche, F. Gelis, H. Zaraket, and R. Kobes,
Phys. Rev. D. {\bf 58}, 085003 (1998).

\bibitem{MT} D. Dutta et al. and P. Aurenche et al. Private Communication,
F. D. Steffen and M. H. Thoma, hep-ph/0103044.

\end{thebibliography}


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\caption{   Same as Fig.~1, with the radiations from the
quark-matter evaluated to the order of two loops. The contribution
of the quark-matter is corrected for the factor of 4 (\protect\cite{MT}).
(This replaces the earlier Fig.~1.)
}
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nucl-th0103022.extracted_bib
\begin{thebibliography}{37}

\bibitem{pat} P. Aurenche, F. Gelis, H. Zaraket, and R. Kobes,
Phys. Rev. D. {\bf 58}, 085003 (1998).

\bibitem{MT} D. Dutta et al. and P. Aurenche et al. Private Communication,
F. D. Steffen and M. H. Thoma, hep-ph/0103044.

\end{thebibliography}