If it were so easy to get out of the false-vacuum state, we wouldn't be here.
While it's in principle possible to create a localized vacuum state which has electroweak phase transition parameters which differ from the vacuum parameters, that state will always decay. The only way it wouldn't decay would be if the localized vacuum state was of lower energy, a state which would then spread at nearly the speed of light, destroying the entire observable universe.
The fact that this has not happened within the last 14 billion years means that there must be a potential energy barrier high enough to:
a) Prevent tunneling of the vacuum state to the true vacuum anywhere in our past lightcone over the last 14 billion years.
b) Prevent even the highest-energy particle interactions from producing energies high enough to get over the barrier.
As we've observed particle collisions with energies as high as ##10^{21} eV##, the potential barrier to kick us out of the false vacuum must be much higher than that (if we are in a false vacuum). Quantum vacuum decay limits may show it has to be even higher.