In the present work, we study minimizers of the Landau-de Gennes free energy
in a bounded domain Ω⊂R3. We prove that at low
temperature minimizers do not vanish, even for topologically non-trivial
boundary conditions. This is in contrast with a simplified Ginzburg-Landau
model for superconductivity studied by Bethuel, Brezis and H\'elein. Merging
this with an observation of Canevari we obtain, as a corollary, the occurence
of biaxial escape: the tensorial order parameter must become strongly biaxial
at some point in Ω. In particular, while it is known that minimizers
cannot be purely uniaxial, we prove the much stronger and physically relevant
fact that they lie in a different homotopy class