  A new mechanism for chiral symmetry restoration at extreme high magnetic
fields is proposed in the context of the Magnetic Catalysis scenario in Weyl
Semimetals. Contrary to previous proposals, here we show that, at very large
magnetic fields, the transverse velocity of the axion field, the phase mode of
the chiral condensate $\langle \bar{\Psi}\Psi\rangle$, becomes effectively
one-dimensional and its fluctuations destroy a possible nonzero value of this
fermionic condensate. We also show that, despite of the $U(1)$ chiral symmetry
not being broken at extremely large magnetic fields, the spectrum of the system
is comprised by a well defined gapless bosonic excitation, connected to the
axion mode, and a correlated insulating fermionic liquid that is neutral to
$U(1)$ chiral transformations. When the theory is supplemented with the
inclusion of dynamical electromagnetic fields, the chiral symmetry is broken
again, and the conventional scenario of magnetic catalysis can be recovered.
