Single-molecule
magnets (SMMs) are expected to be promising candidates
for the applications of high-density information storage materials
and quantum information processing. Lanthanide SMMs have attracted
considerable interest in recent years due to their excellent performance.
It has always been interesting but not straightforward to study the
relaxation and blocking mechanisms by embedding 3d ions into 4f SMMs.
Here we report a family of air-stable 3d–4f ion-pair compounds,
YFe (1), DyCr (2), DyFe (3),
DyCo (4), and Dy0.04Y0.96Fe (5), composed of pentagonal bipyramidal (D
5h
) LnIII cations and transition
metallocyanate anions. The ion-pair nature makes the dipole–dipole
interactions almost the only component of the magnetic interactions
that can be clarified and analytically resolved under proper approximation.
Therefore, this family provides an intuitive opportunity to investigate
the effects of 3d–4f and 4f–4f magnetic interactions
on the behavior of site-resolved 4f SMMs. Dynamic magnetic measurements
of 1 under a 4 kOe external field reveal slow magnetic
relaxation originating from the isolated [FeIII]LS (S = 1/2) ions. Under zero
dc field, compounds 2–5 show similar magnetic
relaxation processes coming from the separated pentagonal bipyramidal
(D
5h
) DyIII ions with high Orbach barriers of 592(5), 596(4), 595(3), and 606(4)
K, respectively. Comparatively, both compounds 3 and 5 exhibit two distinct relaxation processes, respectively
from the [FeIII]LS and DyIII [U
eff = 596(4) K for 3 and 610(7)
K for 5] ions, under a 4 kOe dc field. The dipolar
interactions between the neighboring TMIII (TM = transition
metal, CrIII or [FeIII]LS) and DyIII ions were revealed to have little effect on the thermal
relaxation in compounds 2, 3, and 5, or the coexistence of the two separate relaxation processes
in compounds 3 and 5 under a 4 kOe dc field,
but they significantly affect the quantum tunneling of magnetization
and the magnetic hysteresis behavior of 2 and 3 at low temperatures compared to those of 4.