Abstract

The reactions of hydrated lanthanide(III) [Ln(III)] nitrates and salicylideneaniline (salanH) have provided access to two families of mononuclear complexes depending on the reaction solvent used. In MeCN, the products are [Ln(NO3)3(salanH)2(H2O)]·MeCN, and, in MeOH, the products are [Ln(NO3)3(salanH)2(MeOH)]·(salanH). The complexes within each family are proven to be isomorphous. The structures of complexes [Ln(NO3)3(salanH)2(H2O)]·MeCN (Ln = Eu, 4·MeCN_Eu, Ln = Dy, 7·MeCN_Dy; Ln = Yb, 10·MeCN_Yb) and [Ln(NO3)3(salanH)2(MeOH)]·(salanH) (Ln = Tb, 17_Tb; Ln = Dy, 18_Dy) have been solved by single-crystal X-ray crystallography. In the five complexes, the LnIII center is bound to six oxygen atoms from the three bidentate chelating nitrato groups, two oxygen atoms from the two monodentate zwitterionic salanH ligands, and one oxygen atom from the coordinated H2O or MeOH group. The salanH ligands are mutually “cis” in 4·MeCN_Eu, 7·MeCN_Dy and 10·MeCN_Yb while they are “trans” in 17_Tb and 18_Dy. The lattice salanH molecule in 17_Tb and 18_Dy is also in its zwitterionic form with the acidic H atom being clearly located on the imine nitrogen atom. The coordination polyhedra defined by the nine oxygen donor atoms can be described as spherical tricapped trigonal prisms in 4·MeCN_Eu, 7·MeCN_Dy, and 10·MeCN_Yb and as spherical capped square antiprisms in 17_Tb and 18_Dy. Various intermolecular interactions build the crystal structures, which are completely different in the members of the two families. Solid-state IR data of the complexes are discussed in terms of their structural features. 1H NMR data for the diamagnetic Y(III) complexes provide strong evidence that the compounds decompose in DMSO by releasing the coordinated salanH ligands. The solid complexes emit green light upon excitation at 360 nm (room temperature) or 405 nm (room temperature). The emission is ligand-based. The solid Pr(III), Nd(III), Sm(III), Er(III), and Yb(III) complexes of both families exhibit LnIII-centered emission in the near-IR region of the electromagnetic spectrum, but there is probably no efficient salanH→LnIII energy transfer responsible for this emission. Detailed magnetic studies reveal that complexes 7·MeCN_Dy, 17_Tb and 18_Dy show field-induced slow magnetic relaxation while complex [Tb(NO3)3(salanH)2(H2O)]·MeCN (6·MeCN_Tb) does not display such properties. The values of the effective energy barrier for magnetization reversal are 13.1 cm−1 for 7·MeCN_Dy, 14.8 cm−1 for 17_Tb, and 31.0 cm−1 for 18_Dy. The enhanced/improved properties of 17_Tb and 18_Dy, compared to those of 6_Tb and 7_Dy, have been correlated with the different supramolecular structural features of the two families. The molecules [Ln(NO3)3(salanH)2(MeOH)] of complexes 17_Tb and 18_Dy are by far better isolated (allowing for better slow magnetic relaxation properties) than the molecules [Ln(NO3)3(salanH)2(H2O)] in 6·MeCN_Tb and 7·MeCN_Dy. The perspectives of the present initial studies in the Ln(III)/salanH chemistry are discussed.

Highlights

  • The interdisciplinary field of Molecular Magnetism [1] has undergone revolutionary changes since the early 1990s when it was discovered that the 3-dimensional metal coordination cluster [Mn12O12(O2CMe)16(H2O)4] could behave as a single-domain tiny magnet at a very low temperature [2,3,4]

  • Solid-state IR data of the complexes are discussed in terms of their structural features. 1H NMR data for the diamagnetic Y(III) complexes provide strong evidence that the compounds decompose in DMSO by releasing the coordinated salanH ligands

  • The coordination numbers that give rise to strong axial crystal fields are 1 and 2. Such Ln(III) complexes cannot be isolated, but extensive synthetic and magnetic experimental work has proven that the DyIII coordination number can be higher as long as the strong axial crystal field is supported by equational ligands that are weak donors

Read more

Summary

Introduction

The interdisciplinary field of Molecular Magnetism [1] has undergone revolutionary changes since the early 1990s when it was discovered that the 3-dimensional metal coordination cluster [Mn12O12(O2CMe)16(H2O)4] could behave as a single-domain tiny magnet at a very low temperature [2,3,4]. Such Ln(III) complexes cannot be isolated, but extensive synthetic and magnetic experimental work has proven that the DyIII coordination number can be higher (this is the usual situation) as long as the strong axial crystal field is supported by equational ligands that are weak donors In addition to their exciting magnetic properties, the LnIII ions in their simple salts and complexes give rise to interesting photoluminescence properties arising from forbidden 4f-4f (or 4f-5d in the case of CeIII) electronic transitions [37,38]. Luminescent SIMs are of great scientific value for the in-depth investigation of the mechanisms that govern the magnetization relaxation in mononuclear Ln(III) complexes because photoluminescence studies can, in principle, allow scientists to determine spectroscopically the Stark sublevels of some LnIII ions and compare them with those derived from the magnetic measurements Excellent results on this topic are available in References [44,46,47,48,49]. BBeeffoorreecclloossiinnggtthheeiinnttrroodduuccttiioonn,,wweewwoouullddlliikkeettoossttaatteetthhaatttthheerreeiissccuurrrreennttllyyaarreenneewweeddiinntteerreesstt iinnththeechchememisitsrtyryofomf monoonnounculecaleraLrnL(nII(II)I-IS)c-Shcifhfibffasbeasceomcopmlepxleesxbesecbaeucsaeuosfetowfotwreoasroenass:o(nas):T(hae)rTe hhearse bheaesnbdeeemn odnesmtroantesdtrathteadt ttwhaot atwndo faonudr efoleucrtreolnecstrcoannsbceanstobreedst,orreesdp,ercetisvpeelcyt,ivinelyin, tirnaminotrleacmuolalercaunladr ianntedrminotelercmuolalercCul-aCr Cbo-Cndbsonfodrsmfoedrmbeyd Lbny(LIInI)(-IaIIs)s-iasstesidstereddruecdtuiocntioonf othf ethiemiimnoinogrgoruopupofofSSchchififffbbaassee lliiggaannddss,, wwhhicichhshsohwoswths atththaet latthteer claantteprrocvaidne approrovmidiesinag apltreormnaistiivnegtoaaltmerindaetaivned ctyocloapmenidtaediaenndyl clyigcalonpdesnatnaddioepneynl laignaonvdesl raonudteotpoetnhea rneodvuecltirvoeuctheetmo itshteryreodf ulacntitvheancihdeems [is7t9r]yaonfdla(bn)thYabn(IiIdI)esco[7m9p] laenxdes (wb)itYhbp(oIIlIy)dceonmtaptelecxheeslawtiinthg Spcohliyffdbenastaestearceheqluabtiint gcaSncdhidifaf tbeassdeuseatroe tqhuebvietrcyalnadrgideastpelsitdtiuneg btoettwheeevnetrhye lealregcetrsopnliicttignrgoubnedtwdeoeunbtlheteaenledcttrhoenfiicrsgtreoxucnitdeddocruybslteatl afinedldthsteaftiersatnedxtchiteeidr icnrtyrsintaslicfisellodwstpaateraamndagtnheetiirc irnetlrainxasitciosnlo[w80]paasrawmeallgansetciacnrdeildaxaatetisofnor[8n0o]vaesl wcoeullpalesdcaenledcitdroanteics qfourbnito-nvuelclceoaurpqluedbiet lseycsttreomnisc[q8u1]b.itnuclear qubit systems [81]

Synthetic Comments
Conventional Characterization of the Complexes
C28 C33 cc--CC33C34 cc34c-N6 c
Single-Crystal X-ray Crystallography
Conclusions and Perspectives
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call