A series of mononuclear
DyIII compounds, [Dy(tmpd)3(4,4′-dmpy)]
(1), [Dy(tffb)3(4,4′-dmpy)] (2), [Dy(tffb)3(5,5′-dmpy)] (3), and [Dy(tmpd)3(5,5′-dmpy)] (4)
[tmpd = 4,4,4-trifluoro-1-(4-methoxyphenyl)-1,3-butanedione, tffb
= 4,4,4-trifluoro-1-(4-fluorophenyl)-1,3-butanedione, 4,4′-dmpy
= 4,4′-dimethyl-2,2′-bipyridyl, and 5,5′-dmpy
= 5,5′-dimethyl-2,2′-bipyridyl], have been synthesized
by modifying β-diketonate ligands and capping N-donor co-ligands.
DyIII ions in 1–4 possess N2O6 octacoordinated environments. Compounds 1 and 2 exhibit distorted trigonal dodecahedron configurations,
while 3 and 4 display distorted square antiprismatic
configurations. Systematic investigations of the alternating current
measurements indicate the different magnetic relaxation dynamics with
energy barriers (U
eff) of 66 K (1, 45 cm–1), 189 K, (2, 131
cm–1), 115 K (3, 79 cm–1), and 205 K (4, 142 cm–1). To deeply
understand their different magnetic behaviors, the magnetic anisotropies
of 1–4 were studied by ab initio calculations. From ab initio calculations, the
energies of the first excited state (KD1) are consistent
with the experimental U
eff under zero
direct current field. Compound 4 presents the largest U
eff because of the smallest g
X,Y
and μQTM as well as the most strong axial crystal field parameters
(CFPs) among compounds 1–4. The M versus H data exhibit butterfly-shaped hysteresis
loops at 2 K for 1–4. The different coordination
geometries, the magnetic dynamics, the electrostatic repulsion, and
CFPs result from the different substituent effects of ligands, including
the electronic effect, the steric effect, and the positions of substituted
groups.