We theoretically investigate the generation and Josephson current signatures
of Floquet Majorana end modes (FMEMs) in a periodically driven altermagnet (AM)
heterostructure. Considering a one-dimensional (1D) Rashba nanowire (RNW)
proximitized to a regular
s-wave superconductor and a
d-wave AM, we
generate both
0- and
π-FMEMs by driving the nontopological phase of the
static system. While the static counterpart hosts both topological Majorana
zero modes (MZMs) and non-topological accidental zero modes (AZMs), the drive
can gap out the static AZMs and generate robust
π-FMEMs, termed as
topological AZMs (TAZMs). We topologically characterize the emergent FMEMs via
dynamical winding numbers exploiting chiral symmetry of the system. Moreover,
we consider a periodically driven Josephson junction comprising of RNW/AM-based
1D topological superconduting setup. We identify the signature of MZMs and
FMEMs utilizing
4π-periodic Josephson effect, distinguishing them from
trivial AZMs exhibiting
2π-periodicty, in both static and driven platforms.
This Josephson current signal due to Majorana modes survives even in presence
of finite disorder. Our work establishes a route to realize and identify FMEMs
in AM-based platforms through Floquet engineering and Josephson current
response.