No axion-like particles from core-collapse supernovae?

A strong bound on the properties of axion-like particles (ALPs) has been set by assuming that ALPs are emitted by the protoneutron star just before the core-bounce in Galactic core-collapse supernovae, and that these ALPs subsequently convert to $\gamma$-ray photons which ought to be detected by a $\gamma$-ray mission. This argument has been applied to supernova 1987A to derive the bound on the ALP-photon coupling $g_{a \gamma \gamma} \lesssim 5.3 \cdot 10^{- 12} , {\rm GeV}^{- 1}$foranALPmass$m_a \lesssim 4.4 \cdot 10^{- 10} , {\rm eV}$, and can be applied to the next Galactic supernova to derive the even stronger bound $g_{a \gamma \gamma} \lesssim 2 \cdot 10^{- 13} , {\rm GeV}^{- 1}$foranALPmass$m_a \lesssim 10^{- 9} , {\rm eV}$. We carefully analyze the considered ALP production mechanism and find that it is oversimplified to an unacceptable extent. By taking into account the minimal ingredients required by a realistic analysis, we conclude that the previous results are doomed to failure. As a consequence, all papers quoting the above bound should be properly revised. Yet, since we are unable to rule out the possibility that protoneutron stars emit ALPs, in case a core-collapse supernova explodes in the Galaxy the $\gamma$-ray satellite missions active at that time should look for photons possibly coming from the supernova.