We supplement \ML methods with a \MC simulation to re-investigate the SN1987A
neutrino burst detection by the IMB and Kamiokande experiments. The detector
simulations include background in the the latter and dead-time'' in the former. We consider simple neutrinosphere cooling models, explored previously in the literature, to explore the case for or against neutrino vacuum mixing and massive neutrinos. In the former case, involving kinematically irrelevant masses, we find that the full range of vacuum mixing angles, $0 \le \svac \le 1$, is permitted, and the \ML mixing angle is $\svac = .45.$ In the latter case we find that the inclusion of dead-time’’ reduces previous upper
bounds by 10%, and supplementing the \ML analysis with a \MC goodness-of-fit
test results in a further 15% reduction in the upper limit. Our 95%
C.L. upper limit for is 19.6eV, while the best fit value is 0eV.

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