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We present results from a numerical study of spherically symmetric collapse of a self-gravitating, SU (2) gauge field. Two distinct critical solutions are observed at the threshold of black hole formation. In one case, the critical solution is discretely self-similar, and black holes of arbitrarily small mass can form. However, in the other instance, the critical solution is the n0ex{0ex}=0ex{0ex}1 static Bartnik-Mckinnon sphaleron, and black hole formation turns on at finite mass. The transition between these two scenarios is characterized by the superposition of both types of critical behavior.
Choptuik et al. (Mon,) studied this question.
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