Three cationic [Ln(4)] squares (Ln=lanthanide) were isolated as single crystals and their structures solved as [Dy-4((4)-OH)(HL)(H2L)(3)(H2O)(4)]Cl-2(CH3OH)(4)(H2O)(8) (1), [Tb-4((4)-OH)(HL)(H2L)(3)(MeOH)(4)]Cl-2(CH3OH)(4)(H2O)(4) (2) and [Gd-4((4)-OH)(HL)(H2L)(3)(H2O)(2)(MeOH)(2)]Br-2(CH3OH)(4)(H2O)(3) (3). The structures are described as hydroxo-centered squares of lanthanide ions, with each edge of the square bridged by a doubly deprotonated H2L2- ligand. Alternating current magnetic susceptibility measurements show frequency-dependent out-of-phase signals with two different thermally assisted relaxation processes for 1, whereas no maxima in (M) appears above 2.0K for complex 2. For 1, the estimated effective energy barrier for these two relaxation processes is 29 and 100K. Detailed ab initio studies reveal that complex 1 possesses a toroidal magnetic moment. The ab initio calculated anisotropies of the metal ions in complex 1 were employed to simulate the magnetic susceptibility by using the Lines model (POLY_ANISO) and this procedure yields J(1)=+0.01 and J(2)=-0.01cm(-1) for 1 as the two distinct exchange interactions between the Dy-III ions. Similar parameters are also obtained for complex 1 (and 2) from specific heat measurements. A very weak antiferromagnetic super-exchange interaction (J(1)=-0.043cm(-1) and g=1.99) is observed between the metal centers in 3. The magnetocaloric effect (MCE) was estimated by using field-dependent magnetization and temperature-dependent heat-capacity measurements. An excellent agreement is found for the -S-m values extracted from these two measurements for all three complexes. As expected, 3 shows the largest -S-m variation (23JKg(-1)K(-1)) among the three complexes. The negligible magnetic anisotropy of Gd indeed ensures near degeneracy in the (2S+1) ground state microstates, and the weak super-exchange interaction facilitates dense population of low-lying excited states, all of which are likely to contribute to the MCE, making complex 3 an attractive candidate for cryogenic refrigeration.
Single-Molecule Magnetism, Enhanced Magnetocaloric Effect, and Toroidal Magnetic Moments in a Family of Ln(4) Squares
Affronte Marco;
2015
Abstract
Three cationic [Ln(4)] squares (Ln=lanthanide) were isolated as single crystals and their structures solved as [Dy-4((4)-OH)(HL)(H2L)(3)(H2O)(4)]Cl-2(CH3OH)(4)(H2O)(8) (1), [Tb-4((4)-OH)(HL)(H2L)(3)(MeOH)(4)]Cl-2(CH3OH)(4)(H2O)(4) (2) and [Gd-4((4)-OH)(HL)(H2L)(3)(H2O)(2)(MeOH)(2)]Br-2(CH3OH)(4)(H2O)(3) (3). The structures are described as hydroxo-centered squares of lanthanide ions, with each edge of the square bridged by a doubly deprotonated H2L2- ligand. Alternating current magnetic susceptibility measurements show frequency-dependent out-of-phase signals with two different thermally assisted relaxation processes for 1, whereas no maxima in (M) appears above 2.0K for complex 2. For 1, the estimated effective energy barrier for these two relaxation processes is 29 and 100K. Detailed ab initio studies reveal that complex 1 possesses a toroidal magnetic moment. The ab initio calculated anisotropies of the metal ions in complex 1 were employed to simulate the magnetic susceptibility by using the Lines model (POLY_ANISO) and this procedure yields J(1)=+0.01 and J(2)=-0.01cm(-1) for 1 as the two distinct exchange interactions between the Dy-III ions. Similar parameters are also obtained for complex 1 (and 2) from specific heat measurements. A very weak antiferromagnetic super-exchange interaction (J(1)=-0.043cm(-1) and g=1.99) is observed between the metal centers in 3. The magnetocaloric effect (MCE) was estimated by using field-dependent magnetization and temperature-dependent heat-capacity measurements. An excellent agreement is found for the -S-m values extracted from these two measurements for all three complexes. As expected, 3 shows the largest -S-m variation (23JKg(-1)K(-1)) among the three complexes. The negligible magnetic anisotropy of Gd indeed ensures near degeneracy in the (2S+1) ground state microstates, and the weak super-exchange interaction facilitates dense population of low-lying excited states, all of which are likely to contribute to the MCE, making complex 3 an attractive candidate for cryogenic refrigeration.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
