Ln Centers Research Articles

Cu(II)-Ln(III) (Ln = Gd, Tb and Dy) complexes of an unsymmetrical N2O3 donor ligand: field induced SMM behaviour of Cu(II)-Tb(III) complexes.

Three new hetero-metallic CuII-LnIII complexes [(CuL)Gd(NO3)3(CH3OH)]n (1), [(CuL)Tb(NO3)3(H2O)]·[CuL] (2) and [(CuL)Dy(NO3)3(H2O)]·[CuL] (3) have been synthesized using a mono-nuclear Cu(II) complex, [CuL], of an unsymmetrically di-condensed N2O3 donor Schiff base ligand, N-(3-methoxysalicylidene)-N-(salicylidene)-1,2-ethylenediamine (H2L). Single crystal X-ray crystallography revealed that complex 1 is a nitrate bridged 1D chain of dinuclear Cu(II)-Gd(III) units whereas in 2 and 3, the dinuclear Cu(II)-Ln(III) units are co-crystallized with a [CuL] unit. The Ln(III) centers are nine coordinated with the geometry of a spherical capped square antiprism for Gd and spherical tricapped trigonal prism for Tb and Dy. The geometry of the Cu(II) center is distorted octahedral for complex 1 and distorted square planar for complexes 2 and 3. Temperature-dependent molar magnetic susceptibility measurements in 1-3 revealed the presence of overall ferromagnetic coupling between the Cu(II) and Ln(III) centers. Notably, field induced single-molecule magnet behavior was witnessed in the Tb(III) derivative (2). The ab initio calculations indicated that upon application of an external magnetic field, the tunneling in the ground state of complex 2 gets reduced and thereby field-induced SMM behaviour is observed. Besides, in the case of complex 1, BS-DFT calculations were carried out to gain further insights into the magnetic exchange coupling interactions between the Cu(II) and Gd(III) centers.

Rare‐Earth‐Metal Alkyl and Aryl Compounds in Organic Synthesis

AbstractRare‐earth‐metal (Ln) alkyl and aryl compounds feature highly reactive, thermally labile [Ln−C] σ‐bonds which result in rapid and violent decomposition in the presence of air and moisture. Nevertheless, such [Ln−C] moieties display important intermediate species in numerous organic transformations. Reagents containing [Ln−C] bonds are deliberately generated in situ like Imamoto‐type reagents Ln(III)Cl3/RLi (routinely at low temperatures) or “heavy” lanthanide‐Grignard compounds RLnX. Samarium(III)‐alkyl species are supposed intermediates of SmI2‐promoted Barbier‐type carbon–carbon coupling reactions. Alkyl/aryl ligand exchange at Ln(III) centers has been identified as the crucial step of lanthanide–halogen‐exchange reactions. In the meantime, several such mixed alkyl/halogenido complexes, devoid of an ancillary ligand, could be isolated and scrutinized with regard to structure and reactivity. More recently, Ln(III)‐alkylidene complexes could be accessed, structurally authenticated and successfully employed in Tebbe‐like olefination reactions of ketones.

Formation and Structure of Gas-Phase Lanthanide(III) Cyanobenzyne Complex (η2-4-CNC6H3)LnCl2-, Obtained via Both the Single- and Dual-Ligand Strategies.

The lanthanide(III) cyanobenzyne complexes (η2-4-CNC6H3)LnCl2- (Ln = La-Lu except Eu; Pm was not examined) were generated in the gas phase using an electrospray ionization mass spectrometry coupled with collision-induced dissociation (CID) technique. For all lanthanides except Sm, Eu, and Yb, (4-CNC6H3)LnCl2- can be generated either via a single-ligand strategy through consecutive CO2 and HCl losses of (4-CNC6H4CO2)LnCl3- or via a dual-ligand strategy through successive CO2/C6H5CN or 4-CNC6H4CO2H and CO2 losses of (4-CNC6H4CO2)2LnCl2-. For Sm and Yb, although only reduction products LnCl3- were formed upon CID of (4-CNC6H4CO2)LnCl3-, (4-CNC6H3)LnCl2- were obtained via the dual-ligand strategy without the appearances of other products. CID of (4-CNC6H4CO2)EuCl3- and (4-CNC6H4CO2)2EuCl2- gave EuCl3- and the cyanophenyl complex (4-CNC6H4)EuCl2-, respectively, in both of which the +III oxidation state of Eu was reduced to +II. Density functional theory (DFT) calculations reveal that (4-CNC6H3)LnCl2- are formally described as Ln(III) cyanobenzyne complexes, (η2-4-CNC6H3)LnCl2-, with the dianionic cyanobenzyne ligand (4-CNC6H32-) coordinating to the Ln(III) centers through two Ln-C σ bonds, which is in accordance with their reactivities toward water. Benzyne and substituted benzyne complexes (XC6H3)LuCl2- (X = H, 3-CN, 4-F, 4-Cl, and 4-CH3) were also synthesized in the gas phase via the single- and dual-ligand strategies.

Structures, photoluminescence, and magnetism of 1D lanthanide coordination polymers dominated on 3,5‐dichlorobenzoate

AbstractTwo series of novel coordination polymers (CPs), namely, Ln3(3,5‐DCB)9(bipy) (H2O)2·(bipy) [Ln = Nd (1), Sm (2)] and Ln2(3,5‐DCB)6(bipy)H2O [Ln = Eu (3), Gd (4), Tb (5) and Dy (6)], have been synthesized by hydrothermal reaction of a bridging ligand, 3,5‐dichlorobenzoic acid (3,5‐HDCB), with LnCl3·nH2O and N‐donor neutral ligand, 2,2′‐bipyridine (bipy). Single‐crystal x‐ray diffraction, elemental analysis, IR spectroscopy, thermogravimetric analysis (TGA), and powder x‐ray diffraction (PXRD) for 1–6 are presented. CPs 1 and 2 exhibit trinuclear lanthanide architectures, in which the center Ln(III) are seven‐coordinated and eight‐coordinated adopting monocapped triangular prismatic, distorted square antiprism and bicapped trigonal prismatic coordination geometry, respectively, whereas CPs 3–6 are isostructural dinuclear structures. The center Ln(III) ions are also seven‐coordinated and eight‐coordinated with different coordinate modes adopting distorted monocapped triangular prismatic and square antiprism coordination geometry. Trinuclear CPs 1 and 2 are packed together via hydrogen‐bonding interaction to form the two‐dimensional (2D) supramolecular layers. CPs 3–6 exhibit 2D layers by the π–π interaction. CPs 2, 3, 5, and 6 display the characteristic fluorescent emissions of Sm(III), Eu(III), Tb(III), and Dy(III), respectively. CPs 1 and 4–6 exhibit corresponding weak anti‐ferromagnetic and ferromagnetic interactions of Nd(III), Gd(III), Tb(III), and Dy(III) in the low‐temperature range.

Non‐Classical Early Lanthanide(II) Tris(di‐tert‐butylcyclopentadienyl) Complexes**

AbstractWe report the synthesis of a series of temperature‐sensitive non‐classical early Ln(II) (Ln=lanthanide) complexes, [K(2.2.2‐cryptand)][Ln(Cptt)3] (Cptt=C5H3tBu2‐1,3; 1‐Ln; Ln=La−Nd). Complexes 1‐Ln were typically prepared using Schlenk line techniques rather than more common glove box protocols, by the reduction of the parent Ln(III) complexes [Ln(Cptt)3] (2‐Ln) with KC8 in THF in the presence of 2.2.2‐cryptand at −30 °C. The majority of the 2‐Ln series have been reported previously by the salt metathesis reactions of 3 eq. KCptt with parent LnCl3, and these methods were adapted here to afford 2‐Pr. Complexes 1‐Ln and 2‐Pr were characterized by single crystal XRD, elemental analysis, ATR‐IR and UV‐Vis‐NIR spectroscopy; 1‐La and 2‐Pr were additionally characterized by c.w. EPR spectroscopy, and variable temperature magnetic susceptibility measurements were performed on 2‐Pr. During attempts to synthesize 2‐Nd and 2‐Sm we also obtained small crops of crystals of [Nd(Cptt)2(μ‐I)]2 (3) and [Sm(Cptt)2(μ‐Cl)]2 ⋅ C7H8 (4 ⋅ C7H8), respectively; these complexes were also structurally authenticated, and magnetic data was collected for 4 ⋅ C7H8. The combination of data obtained indicate that the Ln(II) centers in 1‐Ln adopt 4fn5d1 electron configurations, in common with other literature examples of [Ln(CpR)3]− anions (CpR=substituted cyclopentadienyl) for these metals.

Light‐, Middle‐ and Heavy‐Lanthanide Ate‐Complexes Bearing Ln(III)–Si bonds: Structural, Spectroscopic, and Bonding Analysis

Comprehensive SummaryRecent decades have witnessed a rapid development of the lanthanide silicon chemistry. In this research, by reacting [(THF)3LiSiPh3] with Cp3Ln(III)(THF) (Ln(III) = Sm(III), Tb(III), Dy(III), Yb(III)) or Cp2Lu(III)Cl(THF), a series of middle‐ and heavy‐lanthanocene monosilyl/disilyl ate‐complexes ([(DME)3Li][Cp3Ln(III)SiPh3] and [(DME)3Li][Cp2Lu(III)(SiPh3)2]) were synthesized. The structures of the obtained lanthanocene monosilyl/disilyl ate‐complexes were determined by single crystal X‐ray diffraction. Together with the previously reported [(DME)3Li][Cp3La(III)SiPh3] and [(DME)3Li][Cp3Ce(III)SiPh3], a complex group comprising silyl light‐, middle‐ and heavy‐lanthanocene with identical core coordination pattern are presented. The structure analysis of this group of complexes showed that their key geometric parameters, including the Ln(III)–Si bond lengths and Ln(III)–Si–Cph/Cph–Si–Cph angles, were linearly correlated with the ionic radii of Ln(III) centers. Computational studies based on density functional theory calculations suggested the strongly polarized nature of the Ln(III)–Si bonds in these ate‐complexes. The UV‐Vis spectroscopy measurements of this group of ate‐complexes showed that the characteristic absorptions were hypsochromically shifted for complexes with heavier Ln(III) centers. In addition, as revealed by the time‐dependent density functional theory analysis, the HOMOs, in which the Ln(III)–Si σ‐bonding orbitals were the dominant components, of these complexes acted as main donor orbitals in the major electron transitions.

Slow Magnetic Relaxation and Luminescence Properties in Tetra β-Diketonate Lanthanide(III) Complexes

The reaction of [Ln(btfa)3(H2O)2] (btfa- = 4,4,4-trifluoro-1-phenyl-1,3-butanedionate) with additional 4,4,4-trifluoro-1-phenyl-1,3-butanedione (Hbtfa) and acridine (Acr) in ethanol allows the isolation of the mononuclear compounds HAcr[Nd(btfa)4]·EtOH, (1) and HAcr[Ln(btfa)4], Ln = Dy (2) and Yb (3); HAcr+ = acridinium cation. Magnetic measurements indicate that complexes 1–3 show field-induced single-ion magnet behavior with anisotropy energy barriers and preexponential factors of Ueff = 20.7 cm−1, τ0 = 24.5 × 10−8 s; Ueff = 40.5 cm−1, τ0 = 8.6 × 10−10 s and Ueff = 22.7 cm−1, τ0 = 8.4 × 10−8 s, for 1–3 respectively. The solid-state luminescence emission in the NIR region shows efficient energy transfer from the 4,4,4-trifluoro-1-phenyl-1,3-butanedionate ligands to the central Ln3+ ion in the case of compounds 1 and 3.

Regulating Magnetic Relaxation of Radical-Ln-Based Chains Involving Multidentate Nitronyl Nitroxides through Varying Spin Arrangement Motif and Local Symmetry around Ln Centers

The reaction of a newly designed multidentate nitronyl nitroxide radical NIT-Ph-3,5-b-3PyO with Ln(hfac)3·2H2O led to two new 2p–4f chains {[Ln(hfac)3]2(NIT-Ph-3,5-b-3PyO)}n (LnIII = GdIII 1, DyIII 2; NIT-Ph-3,5-b-3PyO = 2-[3,5-bis(3-pyridinyloxy)-phenyl]-4,4,5,5-tetramethylimidazoline-1-oxyl-3-oxide). When the Cu(hfac)2 was introduced in the above reaction, the hetero-tri-spin 2p–3d–4f chains {Ln(hfac)3[Cu(hfac)2]2(NIT-Ph-3,5-b-3PyO)2}n (LnIII = GdIII 3, DyIII 4) were obtained. The crystal data show that the {4f–2p–4f} spin motif is involved in 2p–4f chains, while the {2p–4f–2p} arrangement of spins around Ln centers is found in 2p–3d–4f chains. Direct-current magnetic susceptibility investigations show that both Gd chains display the dominant GdIII–NO ferromagnetic exchanges. Alternating-current susceptibilities prove the existence of the field-induced slow magnetic relaxation behavior in 2, while no nonzero χ″ signals are observed for 4, which could be attributed to the distinct magnetic exchanges originated from different spin arrangements (4f–2p–4f versus 2p–4f–2p) and the different coordination geometry around the DyIII ions for two Dy derivatives (D4d of Dy1 center in 2 and D2d in 4).

α-AsW9O33]9- bridged hexagonal clusters of Ln(III) showing field induced SMM behavior: experimental and theoretical insight.

Polyoxometalates (POM), as inorganic polydentate oxygen donors, provide binding opportunities for oxophilic lanthanide metal centers to construct novel Ln-substituted POM materials with exciting structures and attractive properties. Herein, we have reported four arsenotungstate [α-AsW9O33]9- based lanthanide-containing polyoxometalates [CsxK36-x{Ln6(H2O)12(α-AsW9O33)6}]·yH2O (Ln = Er (1), Gd (2), Ho (3), and Tb (4)), which are synthesized in an alkaline medium. Complexes 1-3 are the dimeric structures of [Ln3(H2O)6(α-AsW9O33)3]18- polyanions, whereas complex 4 is a hexamer of the polyanion [Tb (H2O)2(α-AsW9O33)]6- as a building unit. In all the complexes, [α-AsW9O33]9- units are staggered up and down and give rise to the chair conformation, where one [α-AsW9O33]9- unit bridges two Ln(III) centers through four μ2-oxygen and two terminal oxygen atoms, resulting in the hexagonal arrangement of lanthanides. The dynamic magnetic measurement indicates that only complex 1 exhibits slow relaxation of magnetization with an applied dc field (1500 Oe). To gain insight into the slow relaxation of magnetization in complex 1, the ligand-field parameters and the splitting of the ground-state multiplet of the Er(III) ions have been estimated. The ab initio calculation results confirm that the ground state wave function of these molecules (1, 3, and 4) is mainly composed of a mixture of mJ states, and the non-axial crystal field (CF) terms are more predominant than the axial CF term. The solid-state fluorescence spectra of 1-4 reveal that the photoexcitation O → M ligand-to-metal charge-transfer (LMCT) of arsenotungstate fragments is effectively quenched due to the spatial coordination environment around the Ln(III) ion.

Field-induced SIM behaviour in early lanthanide(III) organophosphates containing 18-crown-6.

Single-ion magnets (SIMs) have attracted wide attention in recent years. Despite tremendous progress in late lanthanide SIMs, reports on early lanthanides exhibiting SIM characteristics are scarce. A series of five novel 18-crown-6 encapsulated mononuclear early lanthanide(III) organophosphates, [{(18-crown-6)Ln(dippH)3}{(18-crown-6)Ln(dippH)2(dippH2)}]·[I3] [Ln = Ce (1), Pr (2), Nd (3)] and [{Ln(18-crown-6)(dippH)2(H2O)}·{I3}] [Ln = Sm (4) and Eu (5)], have been synthesised in the present study. 18-crown-6 coordinates to Ln(III) ions in an equatorial position while the axial positions are occupied by either three phosphate moieties as in 1-3 or two phosphate moieties and one water molecule as in 4 and 5, resulting in a muffin-shaped coordination geometry around the Ln(III) centres. Magnetic susceptibility measurements reveal that Ce and Nd complexes are field-induced single-ion magnets with significant barrier heights. Furthermore, the ab initio CASSCF/RASSI-SO/SINGLE_ANISO calculations on complexes 1 and 3 reveal significant QTM in the ground state rationalising the field-induced single-ion magnetism behaviour of these complexes.

Organometallic Ir(III) complexes: post-synthetic modification, photophysical properties and binuclear complex construction.

Two methods of post-synthetic modification (Suzuki coupling and CuAAC click-reaction) were applied to Ir(III) complexes [Ir(C^N)2N^N]+ to provide the second highly selective donor site. One family of functionalized complexes was used to demonstrate the potential of post-synthetic modification for controlled construction of d-d and d-f binuclear complexes. The complexes obtained were characterized by CHN elemental analysis, NMR spectroscopy, ESI mass-spectrometry, FTIR spectroscopy and single crystal X-ray diffraction analysis. By means of XPS and NEXAFS spectroscopy the coordination of diimine donor site to the Ln(III) centre has been definitely confirmed. The photophysical properties of mono- and binuclear complexes were carefully investigated, and the evolution of luminescent characteristics during the formation of a system of connected metallocenters is also discussed. TDDFT calculations were used to describe the luminescence mechanism and to confirm the conclusions made on the basis of experimental data.

Hybrid Molecular Magnets with Lanthanide- and Countercation-Mediated Interfacial Electron Transfer between Phthalocyanine and Polyoxovanadate.

A series of {V12}-nuclearity polyoxovanadate cages covalently functionalized with one or sandwiched by two phthalocyaninato (Pc) lanthanide (Ln) moieties via V-O-Ln bonds were prepared and fully characterized for paramagnetic Ln = SmIII-ErIII and diamagnetic Ln = LuIII, including YIII. The LnPc-functionalized {V12O32} cages with fully oxidized vanadium centers in the ground state were isolated as (nBu4N)3[HV12O32Cl(LnPc)] and (nBu4N)2[HV12O32Cl(LnPc)2] compounds. As corroborated by a combined experimental (EPR, DC and AC SQUID, laser photolysis transient absorption spectroscopy, and electrochemistry) and computational (DFT, MD, and model Hamiltonian approach) methods, the compounds feature intra- and intermolecular electron transfer that is responsible for a partial reduction at V(3d) centers from VV to VIV in the solid state and at high sample concentrations. The effects are generally Ln dependent and are clearly demonstrated for the (nBu4N)3[HV12O32Cl(LnPc)] representative with Ln = LuIII or DyIII. Intramolecular charge transfer takes place for Ln = LuIII and occurs from a Pc ligand via the Ln center to the {V12O32} core of the same molecule, whereas for Ln = DyIII, only intermolecular charge transfer is allowed, which is realized from Pc in one molecule to the {V12O32} core of another molecule usually via the nBu4N+ countercation. For all Ln but DyIII, two of these phenomena may be present in different proportions. Besides, it is demonstrated that (nBu4N)3[HV12O32Cl(DyPc)] is a field-induced single molecule magnet with a maximal relaxation time of the order 10-3 s. The obtained results open up the way to further exploration and fine-tuning of these three modular molecular nanocomposites regarding tailoring and control of their Ln-dependent charge-separated states (induced by intramolecular transfer) and relaxation dynamics as well as of electron hopping between molecules. This should enable us to realize ultra-sensitive polyoxometalate powered quasi-superconductors, sensors, and data storage/processing materials for quantum technologies and neuromorphic computing.

Windmill-like Ln4 Clusters [Ln = Tb(III) and Dy(III)] Bridged by [α-AsW9O33]9- Unit Showing Zero-Field SMM Behavior: Experimental and Theoretical Investigation.

Herein, two polyoxometalate (POM)-ligated tetranuclear rare-earth metal complexes having the molecular formula [CsxK24-x{Ln4(H2O)8(α-AsW9O33)4}]·yH2O {x = 5, y = 20, and Ln = Tb(III) (1); and x = 6, y = 28, and Ln = Dy(III) (2)} were synthesized by a one-pot reaction with LnCl3·6H2O using di-lacunary [As2W19O67(H2O)]14- precursor and characterized. The structural analysis shows that the building units [α-AsW9O33]9- are bridged by four rare-earth ions, where one [α-AsW9O33]9- bridged two Ln(III) centers asymmetrically by μ2-O and terminal oxygen atoms. The [α-AsW9O33]9- units are orthogonal to each other, resembling as vanes of a windmill. The magnetic studies disclosed the presence of large magnetic anisotropy and slow relaxation of magnetization behavior [Ueff = 15.2 K (1) and 26 K (2)] in the absence of an external magnetic field. Detailed analysis of relaxation dynamics confirmed that the QTM process in 2 (τQTM = 2.50 × 10-4 s) is slower as compared to complex 1 (τQTM = 2.38 × 10-4 s), and the relaxation process mainly follows the shortcut pathways (such as QTM, optical, and acoustic phonon process) rather than the thermally activated Orbach process. Further, the ab initio calculations show high axial ground states with minimum transverse anisotropy and provide a good agreement between calculated and experimental magnetic data for both complexes. It has also been observed that the local symmetry (D4d subgroup) around the metal centers in 1 provides higher axiality and stabilizes mJ = ±6 of Tb(III) more as compared to mJ = ±15/2 of Dy (III) in 2, resulting in higher energy splitting of the ground state in the former complex. The combined experimental and theoretical observations suggest that the high axial nature of the ground state with minimum transverse anisotropy resulting from local ligand field symmetry is responsible for the observed zero-field single-molecule magnet (SMM) behavior in the studied complexes. Notably, complex 1 is the first example of a POM-based terbium complex that shows SMM behavior in the absence of an external field.

Heterometallic {Fe18M6} (M = Y, Gd, Dy) Pivalate Wheels Display Solvent-Induced Polymorphism

A new series of heterometallic wheels, isolated as [Fe18M6(piv)12(Htea)18(tea)6(N3)6]·n(solvent) (MIII = Y (1a, 1b), Gd (2a, 2b), and Dy (3a, 3b); Hpiv = pivalic acid, H3tea = triethanolamine), forms by the reaction of trinuclear μ3-oxo-linked or hexanuclear μ-OH-linked Fe(III) pivalate clusters with rare earth nitrates, H3tea, and azide ligands in MeOH/MeCN or EtOH/MeCN media under ultrasonic irradiation. Single-crystal X-ray diffraction showed that wheels 1a–3a prepared from MeOH/MeCN solutions crystallize in the triclinic space group P1̅ and have Ci symmetry, whereas wheels 1b–3b received from EtOH/MeCN solution crystallize in the trigonal space group R3̅ and have C3i symmetry. Magnetic studies reveal medium antiferromagnetic exchange interactions within the Fe3 trimeric unit (with the exchange coupling parameters of JFe3 = −13.1 cm–1 for 1a, JFe3 = −11.6 cm–1 for 1b) and weak intermolecular antiferromagnetic exchange interactions (λmf = −0.366 mol cm–3 and −0.368 mol cm–3 (zJmf = −0.19 cm–1), respectively). This leads to spin ground states of S = 5/2 for each {Fe3} unit. Substitution of diamagnetic Y(III) centers by paramagnetic Ln(III) centers (in 2a/2b by Gd(III) and in 3a/3b by Dy(III) centers) results in ferromagnetic exchange interactions between the Fe(III) and Ln(III) centers in addition to the predominant antiferromagnetic Fe···Fe interactions in 1a/1b.

Structures and Magnetic Properties of Carbonato-Bridged Hexanuclear NiII4LnIII2 (Ln = Gd, Tb, Dy) Complexes Formed by Atmospheric Carbon Dioxide Fixation in the Absence of an External Base

The reaction of the mononuclear Ni(II) building block [NiL] of an asymmetrically dicondensed N2O3 donor Schiff base ligand, N-salicylidene-N′-3-methoxysalicylidene-1,3-propanediamine (H2L), with LnCl3·6H2O (Ln = Gd, Tb, Dy) in a 2:1 molar ratio leads to the formation of three hexanuclear carbonato-bridged Ni4Ln2 complexes formulated as [Ni4Ln2(CO3)2Cl2(L)2(L′)2(CH3CN)2]·4CH3CN·2H2O (Ln = Tb (2), Dy (3)), where H2L′ = N,N′-bis(salicylidene)-1,3-propanediamine. In complex 1, the unsymmetrical nature of the Schiff base remains intact; however, in 2 and 3, between the two metalloligands coordinated to each Ln, one is the precursor [NiL] of the unsymmetrical ligand whereas the other [NiL′] of the symmetrical ligand, formed by an in situ aldehyde-exchange reaction during complex formation with Ln salts. The Ln(III) centers are octacoordinated with a biaugmented-trigonal-prismatic geometry in all three complexes. In complex 1, half of the Ni(II) centers possess a distorted octahedral geometry while the other half has a square-pyramidal geometry; all of the Ni(II) centers in complexes 2 and 3 have a distorted-octahedral geometry. A magnetic study clarifies that the Ni–Ln magnetic exchange couplings are ferromagnetic. Though the complexes consist of a hexanuclear [Ln2Ni4] system, the magnetic properties have been analyzed on a trinuclear Ni–Ln–Ni basis. The exchange parameter 2JGd–Ni/kB in 1 was estimated to be +0.61 to +0.84 K across the double-oxide bridges. Complexes 2 and 3 exhibited an indication of single-molecule magnets in an ac susceptibility study.

Giant Ln 30 -Cluster-Embedded Polyoxotungstate Nanoclusters with Exceptional Proton-Conducting and Luminescent Properties

Giant Ln ₃₀ -Cluster-Embedded Polyoxotungstate Nanoclusters with Exceptional Proton-Conducting and Luminescent Properties

Magneto-thermal and magnetization relaxation dynamics of a family of di-nuclear lanthanide complexes

The reaction of Ln(NO3)3·nH2O (where Ln = Gd, Tb, Dy or Yb) in the presence of sodium acetate led us to isolate a family of structurally analogous dinuclear lanthanide complexes with the general molecular formula of [Ln2(CH3COO)4(NO3)2(H2O)4]. 2H2O (where Ln = Gd (1) or Tb (2) or Dy (3) or Yb (4)), which are characterized by single-crystal X-ray diffraction. The dc magnetic susceptibility measurements were performed on 1 reveal the presence of a weak ferromagnetic exchange between the Gd(III) center (J = +0.01 cm−1; −2JS1.S2 Hamiltonian). This weak exchange interaction in 1 is presumably overcome by the external magnetic field, and therefore, the X-band EPR spectral features of 1 were simulated by considering the single-ion spin Hamiltonian parameter (g = 1.98, D = 0.03 cm−1, and ∣E/D∣= 0.004). In contrast to 1, complexes 2–4 exhibit a weak antiferromagnetic exchange between the Ln(III) centers. The magnetization relaxation dynamics studies performed on the anisotropic complexes (2–4) show slow relaxation of magnetization in the presence of an optimum external magnetic field. The spin–lattice relaxation predominantly follows the Direct and Raman mechanism exclusively, and the Orbach process was found to be non-existent. By employing ab initio calculations, the electronic structure and the mechanism of magnetization relaxation dynamics of 2–4 have been investigated. The magnetocaloric effect parameter for 1 shows a change in magnetic entropy (−ΔSm) value of 39 J Kg−1 K−1 at 2.0 K (ΔH = 70 kOe), which is one of the largest −ΔSm value registered among the various discrete molecular coolants reported in the literature..

Solvothermal self assembly of three lanthanide(III)-succinates: Crystal structure, topological analysis and DFT calculations on water channel

Three new coordination polymers have been assembled by self-assembly of lanthanide(III) ions and succinic acid in dimethylformamide–water (DMF-H2O) mixed solvent having formulae; {[Ln(suc)1.5(H2O)2]•xH2O}n; (1), (2) and (3) [Where Ln = La (1), Pr (2) and Nd (3), suc = succinate dianion; x = 2 for CP 1, x = 1 for CP 2 and x = 4 for CP 3]. In all three coordination polymers (CPs) 1-3, the Ln(III) centres are ten coordinated with bicapped square antiprismatic geometry (SAPRS-10). Crystallographic analysis reveals that CPs 1-3 crystallize in triclinic system P¯1 space group. The linker succinic acid displays two different bonding modes: (μ2-κ4, η2:η2) and (μ4-κ6, η1:η2:η2:η1). All CPs 1-3 are isostructural and isomorphous. The two Ln centres in CPs 1-3 are bridged together through succinate anions via (μ4-κ6, η1:η2:η2:η1) mode forming dinuclear (Ln2O18) Secondary building unit (SBU) which are extended infinitely to generate one-dimensional chains. These 1D chains are further extended along the b-axis to form two-dimensional layered structures via (μ2-κ4, η2:η2) mode and finally three-dimensional network. In case of Nd, the quality of the crystal allows to locate a major number of lattice water molecules (x = 4) than in the other two complexes and, remarkably, the formation of water channels can be realized and studied. It has been analyzed using DFT calculations combined with the molecular electrostatic potential (MEP) surfaces, the quantum theory of “atoms-in-molecules” QTAIM and non–covalent interaction index (NCIplot) analyses.

XeF2 Coordination to La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy and Y in Rare‐Earth Metal(III) Tetrafluoridoborates

AbstractRemoval of volatiles at 243 K from solutions of completely dissolved LnF3 (Ln=La–Dy and Y) and XeF2 (molar ratio 1 : 3) in anhydrous HF acidified with an excess of BF3 resulted in [Ln(XeF2)3](BF4)3 salts. Isolated solids are stable at 298 K and give similar Raman spectra. [La(XeF2)3](BF4)3 crystallizes in the monoclinic space group C2/m at 150 K. Each La atom is coordinated with three XeF2 ligands. Six F atoms provided by six bridging BF4 units, that connect the neighboring La3+ atoms into columns, complete the nine‐fold coordination of each La atom. Chemical reactions carried out in the same way but with molar ratio LnF3 : XeF2=1 : 1 yielded [Ln(XeF2)](BF4)3 salts (La ‐ Nd). Crystal structures of La and Nd salts are isotypic and crystallize in the monoclinic space group P21/m at 150 K (La) and 200 K (Nd). Each Ln center is coordinated by nine fluorine atoms provided by eight BF4 units and one XeF2 ligand. The BF4 groups interconnect the Ln atoms into two‐dimensional layers. With molar ratio LnF3 : XeF2=1 : 2 and the same synthetic approach, only La yielded [La(XeF2)2](BF4)3 salt. Prolonged pumping of [Ln(XeF2)n](BF4)3 (n=3, 2, 1) at 298 K or attempts of the isolation at 298 K resulted in products with lower content of XeF2 or in mixtures of various products. In addition to [Ln(XeF2)](BF4)3 and LnF3/BF3 products, the [Ln(XeF2)]F(BF4)2 salts (Ln=La, Nd, Sm, Eu, Tb, Dy and Y) also formed. The crystal structures of LaF(HF)(BF4)2 and LaF(BF4)2 side products were determined.

Reduced quenching effect of pyridine ligands in highly luminescent Ln(III) complexes: the role of tertiary amide linkers.

Luminescent Eu(III) and Tb(III) complexes were synthesised from octadentate ligands carrying various carbostyril sensitizing antennae and two bidentate picolinate donors. Antennae were connected to the metal binding site via tertiary amide linkers. Antennae and donors were assembled on a 1,4,7-triazacyclononane (tacn) platform. Solution- and solid-state structures were comparable to those of previously reported complexes with tacn architectures, with nine-coordinate distorted tricapped trigonal prismatic Ln(III) centres, and distinct from those based on 1,4,7,10-tetraazacyclododecane (cyclen) macrocycles. In contrast, the photophysical properties of these tertiary amide tacn-based complexes were more comparable to those of previously reported systems with cyclen ligands, showing efficient Eu(III) and Tb(III) luminescence. This represents an improvement over secondary amide-linked analogues, and is due to a greatly increased sensitization efficiency in the tertiary amide-linked complexes. Tertiary amide-linked Eu(III) and Tb(III) emitters were more photostable than their secondary amide-linked analogues due to the suppression of photoinduced electron transfer and back energy transfer.