posted on 2016-10-13, 14:57authored byTulika Gupta, Mohammad Faizan Beg, Gopalan Rajaraman
Extensive ab initio
CASSCF/RASSI-SO/SINGLE_ANISO/POLY_ANISO calculations have been undertaken
on eight structurally similar previously synthesized [CuII(L)(C3H6O)LnIII(NO3)3] (Ln = Dy (1), Tb (3), Ho
(5), and Er (7)) and [VIVO(L)(C3H6O)LnIII(NO3)3] (Ln = Dy (2), Tb (4), Ho (6), and Er (8)) (here H2L = N,N′-bis(3-methoxysalicylidene)-1,3-diamino-2,2-dimethylpropane)
complexes (crystal structures reported earlier). Our estimated exchange
interactions (J) using the Lines model for complexes 1–8 (1.55 cm–1, 0.15
cm–1, 5.30 cm–1, 0.06 cm–1, 1.05 cm–1, −0.18 cm–1, 0.24 cm–1, and −0.02 cm–1 for complexes 1–8 respectively)
match well with the experimental values (HE-EPR and pulse magnetization
technique) reported earlier and offer confidence in the methodology
employed. We have established the mechanism of magnetic coupling for
this series to rationalize the observation that LnCu complexes are
strongly coupled compared to LnV complexes. Besides, the results procured
based on the BS-DFT method imply a crucial role of overlap between
the 3d and 4f orbitals, the formally empty 5d/6s/6p orbitals of LnIII ion in the exchange coupling mechanism. To probe the origin/absence
of magnetization relaxation observed in these complexes 1–8, both the single-ion and the exchange anisotropy
are analyzed. Our calculations reveal that stronger exchange interaction
quenches the quantum tunnelling of magnetization behavior in these
complexes; however, for LnV complexes the exchange interaction was
too small to offer a large blockade barrier. In the quest to obtain
a stronger exchange interaction, we have assessed several models and
have developed a magneto-structural correlation. An antagonizing behavior
between the JCuDy and Ucal values are noted for the Dy–O–O–Cu
dihedral angle correlation developed on complex 1. This
highlights the subtle nature of the magnetic anisotropy in this class
of complexes and postulates that both the single-ion anisotropy and
the exchange interaction are needed to be targeted simultaneously
to achieve a new generation {3d-4f} single molecule magnets (SMM).