Tara J. Burchell

A Polynuclear Lanthanide Single‐Molecule Magnet with a Record Anisotropic Barrier

Single-molecule magnets (SMMs) continue to be an attractive research field because of their unique and intriguing properties and potential applications in high-density data storage technologies and molecular spintronics. The anisotropic barrier (U) of an SMM is derived from a combination of an appreciable spin ground state (S) and uniaxial Ising-like magneto-anisotropy (D). The magnet-like behavior can be observed by slow relaxation of the magnetization below the blocking temperature. Since the discovery of SMMs in the early 1990s, this assumption has formed the basis for the understanding of the origin of the anisotropic barrier. However, in recent years the development of novel lanthanide-only SMMs that challenge and defy this theory pose a number of questions: How can slow relaxation of the magnetization be observed in a nonmagnetic state complex? Why are large energy barriers seen for mononuclear lanthanide(III) complexes? To answer such important questions, it is vital to investigate novel SMMs with high magnetoanisotropy for which the influence of the large negative D value could result in higher anisotropic barriers. Clearly lanthanide-based polynuclear systems are an important avenue to explore in the pursuit of SMMs with higher anisotropic barriers, because of the strong spin–orbit coupling commonly observed in 4f systems. However, lanthanide-only SMMs are rare. The majority of reported SMMs have been prepared with transition-metal ions, although the recent application of a mixed transition-metal/ lanthanide strategy also yielded many structurally and magnetically interesting systems. The scarcity of lanthanide-only SMMs results from the difficulty in promoting magnetic interactions between the lanthanide ions. The interactions can, however, be enhanced by overlapping bridging ligand orbitals. In addition, fast quantum tunneling of the magnetization (QTM), which is common for lanthanide systems, generally prevents the isolation of SMMs with high anisotropic energy barriers. Our recent work suggests that dysprosium(III) ions may hold the key to obtaining high-blocking-temperature lanthanide-only SMMs. When an appropriate ligand system is employed, it is possible to exploit the large intrinsic magnetoanisotropy, high spin, and reduced QTM that dysprosium(III) ions offer. Recently, we have focused our attention towards the synthesis of dysprosium(III) cluster complexes with 1,2bis(2-hydroxy-3-methoxybenzylidene) hydrazone (H2bmh) and 3-methoxysalicylaldehyde hydrazone (Hmsh) as chelating agents (see Figure S1 in the Supporting Information). This strategy has proven to be successful and has led to a polynuclear lanthanide SMM with a record anisotropic barrier. Herein, we report the synthesis, structure, and magnetism of a tetranuclear dysprosium(III) SMM that exhibits the largest relaxation barrier seen for any polynuclear SMM to date. A suspension of DyCl3·6H2O and o-vanillin (2:1 ratio) in DMF/CH2Cl2 (1:5 ratio) was treated with 4 equivalents of Et3N. The solution was stirred for 1 minute, and then 4 equivalents of N2H4·H2O was added. The resulting yellow solution yielded rectangular, orange-yellow crystals of the tetranuclear complex [Dy4(m3-OH)2(bmh)2(msh)4Cl2] (1) in 19.1% yield after 2 days. The msh and bmh ligands were formed in situ by the reaction of o-vanillin and hydrazine. The slight excess of hydrazine is essential for the formation of both ligands; when an excess of o-vanillin was used instead, no product was isolated. The basic conditions promote the deprotonation of the ligands and the formation of bridging hydroxide anions. Single-crystal X-ray analysis revealed the centrosymmetric complex 1 (Figure 1), which has a defect-dicubane central core. The four coplanar Dy ions are bridged by two m3-OH ligands displaced above and below (0.922 ) the Dy4 plane with Dy O bond lengths of 2.362(6), 2.302(6), and 2.447(6) andDy O Dy angles of 106.5(2), 107.7(2), and 105.7(2)8, and also by a combination of four phenoxide oxygen atoms [Dy O 2.312(2), 2.298(6), 2.448(6), 2.345(6) ] and two diaza bridging groups [Dy N 2.508(8), 2.564(8) ]. Close inspection of the packing arrangement reveals stacking of the [*] P.-H. Lin, Dr. T. J. Burchell, Dr. M. Murugesu Chemistry Department, University of Ottawa and Centre for Catalysis Research and Innovation D’Iorio Hall, 10 Marie Curie, Ottawa, ON, K1N6N5 (Canada) Fax: (+1)613-562-5170 E-mail: m.murugesu@uottawa.ca Homepage: http://www.science.uottawa.ca/~mmuruges/

Dinuclear Dysprosium(III) Single-Molecule Magnets with a Large Anisotropic Barrier†

Due to the large intrinsic magnetic anisotropy of the lanthanide ions, rare-earth metal systems, and in particular dysprosium (Dy) based materials, have sparked increasing interest in the area of molecular magnetism. In a molecular complex, when such a unique property is combined with a high-spin ground state (S), slow relaxation of the magnetization can be obtained as seen for single-molecule magnets (SMMs). Although, a number of mixed transition-metal/ lanthanide SMMs have been reported, pure lanthanide SMMs are relatively scarce. The latter molecules are rare owing to the difficulty in promoting magnetic interactions in these systems. These interactions are attained by the overlap of bridging ligand orbitals with the 4f orbitals of the lanthanide ions. Thus, ligand design is one of the key components for achieving such interactions in pure lanthanide-based systems. To induce significant magnetic interaction between the lanthanide ions and synthesize high-energy-barrier SMMs, we have been investigating the use of (2-hydroxy-3-methoxyphenyl)methylene (isonicotino)hydrazine (H2hmi) as a rigid chelate in lanthanide chemistry. Such a linear ligand provides O,N,O,O-based multichelating sites that are especially favorable for lanthanide ion complex formation. They can form dinuclear systems using the bridging phenoxide oxygen atom, and the pyridine group promotes the formation of extended networks that can control the organization of the SMM units in the three-dimensional structure. Herein we report the use of the H2hmi ligand to design materials based on ferromagnetically coupled dinuclear dysprosium(III) SMMs with large relaxation barriers. [Dy2(hmi)2(NO3)2(MeOH)2] (1) and [Dy2(hmi)2(NO3)2 (MeOH)2]1·MeCN (2·MeCN) were obtained from a suspension of Dy(NO3)3·5H2O / H2hmi in methanol (treated with triethylamine) and in a 3:1 mixture of acetonitrile and methanol (treated with pyridine), respectively. After two days, pale orange single crystals were obtained, which were kept in contact with the mother liquor to prevent deterioration. Complexes 1 (Figure 1) and 2 (Figure 2) crystallize in monoclinic P21/c and orthorhombic Pbca space groups, respectively. Both complexes have similar dinuclear

Linking high anisotropy Dy-3 triangles to create a Dy-6 single-molecule magnet

A unique Dy(III)(6) complex is created by linking of two Dy(III)(3) triangles, in which intramolecular ferromagnetic interactions and single-molecule magnetic behaviour have been observed.

Two-dimensional networks of lanthanide cubane-shaped dumbbells.

The syntheses, structures, and magnetic properties are reported for three new lanthanide complexes, [Ln(III)(4)(mu(3)-OH)(2)(mu(3)-O)(2)(cpt)(6)(MeOH)(6)(H(2)O)](2) (Ln = Dy (1.15MeOH), Ho (2.14MeOH), and Tb (3.18MeOH)), based on 4-(4-carboxyphenyl)-1,2,4-triazole ligand (Hcpt). The three complexes were confirmed to be isomorphous by infrared spectroscopy and single-crystal X-ray diffraction. The crystal structure of 1 reveals that the eight-coordinate metal centers are organized in two cubane-shaped moieties composed of four Dy(III) ions each. All metal centers in the cubane core are bridged by two mu(3)-oxide and two mu(3)-hydroxide asymmetrical units. Moreover, each cubane is linked to its neighbor by two externally coordinating ligands, forming the dumbbell {Dy(III)(4)}(2) moiety. Electrostatic interactions between the ligands of the triazole-bridged dimers form an extended supramolecular two-dimensional arrangement analogous to a metal-organic framework with quadrilateral spaces occupied by ligands from axial sheets and by four solvent molecules. The magnetic properties of the three compounds have been investigated using dc and ac susceptibility measurements. For 1, the static and dynamic data corroborate the fact that the {Dy(III)(4)} cubane-shaped core exhibits slow relaxation of its magnetization below 5 K associated with a single-molecule magnet behavior.

Capturing In+ Monomers in a Neutral Weakly Coordinating Environment

The application of a new bis(imino)pyridine ligand allowed the isolation and characterization of [{2,4-(t)Bu(2)C(6)H(3)N=CPh}(2)(NC(5)H(3))]In(+)(OTf)(-) as the first low-valent, main-group metal complex of this ligand scaffold. Structural analysis revealed a unique monomeric In(I) species with a surprisingly long metal-ligand bond. In conjunction with a density functional theory investigation, this complex is shown to display only nominal donor-acceptor interactions between the metal and the neutral ligand. The mixing of the occupied 5s metal orbital with the occupied ligand orbitals reduces the reactivity of the central atom and thus stabilizes this species. An In(III) species, [{2,4-(t)Bu(2)C(6)H(3)N=CPh}(2)(NC(5)H(3))]InCl(2)(+)InCl(4)(-) was also isolated and structurally characterized utilizing this ligand frame.

Synthesis, characterisation and computational studies on a novel one-dimensional arrangement of Schiff-base Mn3 single-molecule magnet

The syntheses, structures and magnetic properties are reported for three new manganese complexes containing the Schiff-base ((2-hydroxy-3-methoxyphenyl)methylene)isonicotinohydrazine (H(2)hmi) ligand. Complex [Mn(II)(H(2)hmi)(2)(MeOH)(2)Cl(2)] (1) was obtained from the reaction of H(2)hmi with MnCl(2) in a MeOH-MeCN mixture. Addition of triethylamine to the previous reaction mixture followed by diethyl ether diffusion yielded a dinuclear manganese [Mn(III)(2)(hmi)(2)(OMe)(2)](infinity).2MeCN.2OEt(2) (2) compound. Upon increasing the MnCl(2)/H(2)hmi ratio, the mixed valence complex [Mn(III)(2)Mn(II)(hmi)(2)(OMe)(2)Cl(2)](infinity).MeOH (3) was obtained. Dc and ac magnetic measurements were carried out on all three samples. The ac susceptibility and field dependence of the magnetisation measurements confirmed that complex 3 exhibits a single-molecule magnet behaviour with an effective energy barrier of 8.1 K and an Arrhenius pre-exponential factor of 3 x 10(-9) s.

Gradual spin crossover behaviour in a linear trinuclear FeII complex

The synthesis, structures and magnetic properties of a new trinuclear spin crossover complex, [FeII3(npt)6(EtOH)4(H2O)2](ptol)6·4EtOH (1), and of its CoII (2 and 3) and NiII (4) analogues, are reported here. The complexes were synthesized by reacting a 1,2,4-triazole-based ligand, 4-(4′-nitrophenyl)-1,2,4-triazole (npt), with the p-tolylsulfonate (ptol) metal salts in methanol or ethanol. Structural analyses revealed that all complexes are iomorphous and consist of a linear trinuclear core where metal centres are bridged by triazole groups. For 1, dc susceptibility measurements exhibit gradual spin transition with T1/2 = 148 K which corresponds to HS → LS crossover for the triazole bridged central FeII ion. This spin transition was confirmed by Single-Crystal X-Ray Diffraction data of 1 at 100 K and 181 K, where the low temperature measurement revealed a decrease in volume for the central FeII ion, which is in agreement with a HS → LS transition.

Turning on Single-Molecule Magnet Behavior in a Linear {Mn3} Compound

The synthesis, structure, and magnetic properties are reported for a new manganese compound with a mixed-valent {Mn(3)} core arranged in a linear fashion. The previously reported complex 1, [Mn(IV)(3)(dpo)(6)]·2MeCN, where H(2)dpo is (E)-1-hydroxy-1,1-diphenylpropan-2-one oxime, served as a starting point for the isolation of a {Mn(3)} compound with an analogous core arrangement through the reaction of Mn(OAc)(2)·4H(2)O, H(3)oxol ((E)-2,5-dihydroxy-2,5-dimethylhexan-3-one oxime), and NaOH in MeOH and MeCN. By using these reaction conditions, compound 2, Na[Mn(IV)(2)Mn(III)(Hoxol)(6)](n)·MeOH·H(2)O, was successfully isolated revealing a central Mn(III) ion thereby introducing structural and magnetic anisotropy to the system. The structure of 2 reveals linear trinuclear Mn(IV)-Mn(III)-Mn(IV) units connected through Na(+) ions forming a linear one-dimensional coordination polymer. The Jahn-Teller axes of each trinuclear unit are aligned parallel within the same chain and form a 75° angle between the two symmetry related chains. Magnetic susceptibility measurements of 1 and 2 in the temperature range 1.9-300 K reveal that only the reduced compound, 2, is a single-molecule magnet (SMM) largely due to the anisotropy introduced by the Jahn-Teller distortions on the Mn(III) ions, which effectively induce this magnet behavior. Weak antiferromagnetic interactions along the chains through the Na(+) cations lead to a modulation of the intrinsic properties of the Mn(IV)-Mn(III)-Mn(IV) SMMs.