  We revisit the uniaxially strained graphene immersed in a uniform homogeneous
magnetic field orthogonal to the layer in order to describe the time evolution
of coherent states build from a semi-classical model. We consider the symmetric
gauge vector potential to render the magnetic field, and we encode the tensile
and compression deformations on an anisotropy parameter $\zeta$. After solving
the Dirac-like equation with an anisotropic Fermi velocity, we define a set of
matrix ladder operators and construct electron coherent states as eigenstates
of a matrix annihilation operator with complex eigenvalues. Through the
corresponding probability density, we are able to study the anisotropy effects
on these states on the $xy$-plane as well as their time evolution. Our results
show clearly that the quasi-period of electron coherent states is affected by
the uniaxial strain.
