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Certain phase transitions between topological quantum field theories (TQFT) are driven by the condensation of bosonic anyons. However, as bosons in a TQFT are themselves nontrivial collective excitations, there can be topological obstructions that prevent them from condensing. Here we formulate such an obstruction in the form of a no-go theorem. We use it to show that no condensation is possible in SO(3) TQFTs with odd . We further show that a layered theory obtained by tensoring SO(3) TQFT with itself any integer number of times does not admit condensation transitions either. This includes (as the case ) the noncondensability of any number of layers of the Fibonacci TQFT.

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