A crystallographically
heterogeneous interface was fabricated by
growing hexagonal graphene (Gr) using chemical vapor deposition (CVD)
on a tetragonal FePd epitaxial film grown by magnetron sputtering.
FePd was alternately arranged with Fe and Pd in the vertical direction,
and the outermost surface atom was identified primarily as Fe rather
than Pd. This means that FePd has a high degree of
L
1
0
-ordering, and the outermost Fe bonds to the carbon
of Gr at the interface. When Gr is grown by CVD, the crystal orientation
of hexagonal Gr toward tetragonal
L
1
0
-FePd
selects an energetically stable structure based on the van der Waals
(vdW) force. The atomic relationship of Gr/
L
1
0
-FePd, which is an energetically stable interface, was unveiled
theoretically and experimentally. The Gr armchair axis was parallel
to FePd [100]
L
10
, where Gr was under a
small strain by chemical bonding. Focusing on the interatomic distance
between the Gr and FePd layers, the distance was theoretically and
experimentally determined to be approximately 0.2 nm. This shorter
distance (≈0.2 nm) can be explained by the chemisorption-type
vdW force of strong orbital hybridization, rather than the longer
distance (≈0.38 nm) of the physisorption-type vdW force. Notably,
depth-resolved X-ray magnetic circular dichroism analyses revealed
that the orbital magnetic moment (
M
l
)
of Fe in FePd emerged at the Gr/FePd interface (@inner FePd:
M
l
= 0.16 μ
B
→ @Gr/FePd
interface:
M
l
= 0.32 μ
B
). This interfacially enhanced
M
l
showed
obvious anisotropy in the perpendicular direction, which contributed
to interfacial perpendicular magnetic anisotropy (IPMA). Moreover,
the interfacially enhanced
M
l
and interfacially
enhanced electron density exhibited robustness. It is considered that
the shortening of the interatomic distance produces a robust high
electron density at the interface, resulting in a chemisorption-type
vdW force and orbital hybridization. Eventually, the robust interfacial
anisotropic
M
l
emerged at the crystallographically
heterogeneous Gr/
L
1
0
-FePd interface. From
a practical viewpoint, IPMA is useful because it can be incorporated
into the large bulk perpendicular magnetic anisotropy (PMA) of
L
1
0
-FePd. A micromagnetic simulation assuming
both PMA and IPMA predicted that perpendicularly magnetized magnetic
tunnel junctions (p-MTJs) using Gr/
L
1
0
-FePd could realize 10-year data retention in a small recording layer
with a circular diameter and thickn...