10 research outputs found
Hydroxide-Free Cubane-Shaped Tetranuclear [Ln<sub>4</sub>] Complexes
The
reaction of the lanthanide(III) chloride salts [Gd(III), Tb(III),
and Dy(III)] with a new chelating, flexible, and sterically unencumbered
multisite coordinating compartmental Schiff-base ligand (<i>E</i>)-2-((6-(hydroxymethyl)pyridin-2-yl)methyleneamino)phenol (LH<sub>2</sub>) and pivalic acid (PivH) in the presence of triethylamine
(Et<sub>3</sub>N) affords a series of tetranuclear Ln(III) coordination
compounds, [Ln<sub>4</sub>(L)<sub>4</sub>(μ<sub>2</sub>-η<sup>1</sup>η<sup>1</sup>Piv)<sub>4</sub>]·<i>x</i>H<sub>2</sub>O·<i>y</i>CH<sub>3</sub>OH (<b>1</b>, Ln = Gd(III), <i>x</i> = 3, <i>y</i> = 6; <b>2</b>, Ln = Tb(III), <i>x</i> = 6, <i>y</i> = 2; <b>3</b>, Ln = Dy(III), <i>x</i> = 4, <i>y</i> = 6). X-ray diffraction studies reveal that the molecular
structure contains a distorted cubane-like [Ln<sub>4</sub>(μ<sub>3</sub>-OR)<sub>4</sub>]<sup>+8</sup> core, which is formed by the
concerted coordination action of four dianionic L<sup>2–</sup> Schiff-base ligands. Each lanthanide ion is eight-coordinated (2N,
6O) to form a distorted-triangular dodecahedral geometry. Alternating
current susceptibility measurements of complex <b>3</b> reveal
frequency- and temperature-dependent two-step out-of-phase signals
under zero direct current (dc) field, which is characteristic of single-molecule
magnet behavior. Analysis of the dynamic magnetic data under an applied
dc field of 1000 Oe to fully or partly suppress the quantum tunneling
of magnetization relaxation process affords the anisotropic barriers
and pre-exponential factors: Δ/<i>k</i><sub>B</sub> = 73(2) K, τ<sub>0</sub> = 4.4 × 10<sup>–8</sup> s; Δ/<i>k</i><sub>B</sub> = 47.2(9) K, τ<sub>0</sub> = 5.0 × 10<sup>–7</sup> s for the slow and fast
relaxations, respectively
<i>Rhombus</i>-Shaped Tetranuclear [Ln<sub>4</sub>] Complexes [Ln = Dy(III) and Ho(III)]: Synthesis, Structure, and SMM Behavior
The reaction of a new hexadentate
Schiff base hydrazide ligand
(LH<sub>3</sub>) with rare earth(III) chloride salts in the presence
of triethylamine as the base afforded two planar tetranuclear neutral
complexes: [{(LH)<sub>2</sub>Dy<sub>4</sub>}(μ<sub>2</sub>-O)<sub>4</sub>](H<sub>2</sub>O)<sub>8</sub>·2CH<sub>3</sub>OH·8H<sub>2</sub>O (<b>1</b>) and [{(LH)<sub>2</sub>Ho<sub>4</sub>}(μ<sub>2</sub>-O)<sub>4</sub>](H<sub>2</sub>O)<sub>8</sub>·6CH<sub>3</sub>OH·4H<sub>2</sub>O (<b>2</b>). These neutral complexes
possess a structure in which all of the lanthanide ions and the donor
atoms of the ligand remain in a perfect plane. Each doubly deprotonated
ligand holds two Ln(III) ions in its two distinct chelating coordination
pockets to form [LH(Ln)<sub>2</sub>]<sup>4+</sup> units. Two such
units are connected by four [μ<sub>2</sub>-O]<sup>2–</sup> ligands to form a planar tetranuclear assembly with an Ln(III)<sub>4</sub> core that possesses a rhombus-shaped structure. Detailed
static and dynamic magnetic analysis of <b>1</b> and <b>2</b> revealed single-molecule magnet (SMM) behavior for complex <b>1.</b> A peculiar feature of the χ<sub>M</sub>″ versus
temperature curve is that two peaks that are frequency-dependent are
revealed, indicating the occurrence of two relaxation processes that
lead to two energy barriers (16.8 and 54.2 K) and time constants (τ<sub>0</sub> = 1.4 × 10<sup>–6</sup> s, τ<sub>0</sub> = 7.2 × 10<sup>–7</sup> s). This was related to the
presence of two distinct geometrical sites for Dy(III) in complex <b>1</b>
<i>Rhombus</i>-Shaped Tetranuclear [Ln<sub>4</sub>] Complexes [Ln = Dy(III) and Ho(III)]: Synthesis, Structure, and SMM Behavior
The reaction of a new hexadentate
Schiff base hydrazide ligand
(LH<sub>3</sub>) with rare earth(III) chloride salts in the presence
of triethylamine as the base afforded two planar tetranuclear neutral
complexes: [{(LH)<sub>2</sub>Dy<sub>4</sub>}(μ<sub>2</sub>-O)<sub>4</sub>](H<sub>2</sub>O)<sub>8</sub>·2CH<sub>3</sub>OH·8H<sub>2</sub>O (<b>1</b>) and [{(LH)<sub>2</sub>Ho<sub>4</sub>}(μ<sub>2</sub>-O)<sub>4</sub>](H<sub>2</sub>O)<sub>8</sub>·6CH<sub>3</sub>OH·4H<sub>2</sub>O (<b>2</b>). These neutral complexes
possess a structure in which all of the lanthanide ions and the donor
atoms of the ligand remain in a perfect plane. Each doubly deprotonated
ligand holds two Ln(III) ions in its two distinct chelating coordination
pockets to form [LH(Ln)<sub>2</sub>]<sup>4+</sup> units. Two such
units are connected by four [μ<sub>2</sub>-O]<sup>2–</sup> ligands to form a planar tetranuclear assembly with an Ln(III)<sub>4</sub> core that possesses a rhombus-shaped structure. Detailed
static and dynamic magnetic analysis of <b>1</b> and <b>2</b> revealed single-molecule magnet (SMM) behavior for complex <b>1.</b> A peculiar feature of the χ<sub>M</sub>″ versus
temperature curve is that two peaks that are frequency-dependent are
revealed, indicating the occurrence of two relaxation processes that
lead to two energy barriers (16.8 and 54.2 K) and time constants (τ<sub>0</sub> = 1.4 × 10<sup>–6</sup> s, τ<sub>0</sub> = 7.2 × 10<sup>–7</sup> s). This was related to the
presence of two distinct geometrical sites for Dy(III) in complex <b>1</b>
Molecular Magnets Based on Homometallic Hexanuclear Lanthanide(III) Complexes
The
reaction of lanthanide(III) chloride salts (Gd(III), Dy(III), Tb(III),
and Ho(III)) with the hetero donor chelating ligand <i>N</i>′-(2-hydroxy-3-methoxybenzylidene)-6-(hydroxymethyl)picolinohydrazide
(LH<sub>3</sub>) in the presence of triethylamine afforded the hexanuclear
Ln(III) complexes [{Ln<sub>6</sub>(L)<sub>2</sub>(LH)<sub>2</sub>}(μ<sub>3</sub>-OH)<sub>4</sub>][MeOH]<sub><i>p</i></sub>[H<sub>2</sub>O]<sub><i>q</i></sub>[Cl]<sub>4</sub>·<i>x</i>H<sub>2</sub>O·<i>y</i>CH<sub>3</sub>OH
(<b>1</b>, Ln = Gd(III), <i>p</i> = 4, <i>q</i> = 4, <i>x</i> = 8, <i>y</i> = 2; <b>2</b>, Ln = Dy(III), <i>p</i> = 2, <i>q</i> = 6, <i>x</i> = 8, <i>y</i> = 4; <b>3</b>, Ln = Tb(III), <i>p</i> = 2, <i>q</i> = 6, <i>x</i> = 10, <i>y</i> = 4; <b>4</b>, Ln = Ho(III), <i>p</i> =
2, <i>q</i> = 6, <i>x</i> = 10, <i>y</i> = 2). X-ray diffraction studies revealed that these compounds possess
a hexanuclear [Ln<sub>6</sub>(OH)<sub>4</sub>]<sup>14+</sup> core
consisting of four fused [Ln<sub>3</sub>(OH)]<sup>8+</sup> subunits.
Both static (dc) and dynamic (ac) magnetic properties of <b>1</b>–<b>4</b> have been studied. Single-molecule magnetic
behavior has been observed in compound <b>2</b> with an effective
energy barrier and relaxation time pre-exponential parameters of Δ/<i>k</i><sub>B</sub> = 46.2 K and τ<sub>0</sub> = 2.85 ×
10<sup>–7</sup> s, respectively
Syntheses, Structures, and Magnetic Properties of a Family of Heterometallic Heptanuclear [Cu<sub>5</sub>Ln<sub>2</sub>] (Ln = Y(III), Lu(III), Dy(III), Ho(III), Er(III), and Yb(III)) Complexes: Observation of SMM behavior for the Dy(III) and Ho(III) Analogues
Sequential reaction of the multisite
coordination ligand (LH<sub>3</sub>) with Cu(OAc)<sub>2</sub>·H<sub>2</sub>O, followed by the addition of a rare-earth(III)
nitrate salt in the presence of triethylamine, afforded a series of
heterometallic heptanuclear complexes containing a [Cu<sub>5</sub>Ln<sub>2</sub>] core {Ln = Y(<b>1</b>), Lu(<b>2</b>),
Dy(<b>3</b>), Ho(<b>4</b>), Er(<b>5</b>), and Yb(<b>6</b>)}. Single-crystal X-ray crystallography reveals that all
the complexes are dicationic species that crystallize with two nitrate
anions to compensate the charge. The heptanuclear aggregates in <b>1</b>–<b>6</b> are centrosymmetrical complexes, with
a hexagonal-like arrangement of six peripheral metal ions (two rare-earth
and four copper) around a central Cu(II) situated on a crystallographic
inversion center. An all-oxygen environment is found to be present
around the rare-earth metal ions, which adopt a distorted square-antiprismatic
geometry. Three different Cu(II) sites are present in the heptanuclear
complexes: two possess a distorted octahedral coordination sphere
while the remaining one displays a distorted square-pyramidal geometry.
Detailed static and dynamic magnetic properties of all the complexes
have been studied and revealed the single-molecule magnet behavior
of the Dy(III) and Ho(III) derivatives
Octanuclear Heterobimetallic {Ni<sub>4</sub>Ln<sub>4</sub>} Assemblies Possessing Ln<sub>4</sub> Square Grid [2 × 2] Motifs: Synthesis, Structure, and Magnetism
Octanuclear
heterobimetallic complexes, [Ln<sub>4</sub>Ni<sub>4</sub>(H<sub>3</sub>L)<sub>4</sub>(μ<sub>3</sub>-OH)<sub>4</sub>(μ<sub>2</sub>-OH)<sub>4</sub>]4Cl·<i>x</i>H<sub>2</sub>O·<i>y</i>CHCl<sub>3</sub> (Dy<sup>3+</sup>, <i>x</i> =
30.6, <i>y</i> = 2 (<b>1</b>); Tb<sup>3+</sup>, <i>x</i> = 28, <i>y</i> = 0 (<b>2</b>) ; Gd<sup>3+</sup>, <i>x</i> = 25.3, <i>y</i> = 0 (<b>3</b>); Ho<sup>3+</sup>, <i>x</i> = 30.6, <i>y</i> = 3 (<b>4</b>)) (H<sub>5</sub>L = <i>N</i><sub>1</sub>,<i>N</i><sub>3</sub>-bis(6-formyl-2-(hydroxymethyl)-4-methylphenol)diethylenetriamine)
are reported. These are assembled by the cumulative coordination action
of four doubly deprotonated compartmental ligands, [H<sub>3</sub>L]<sup>2–</sup>, along with eight exogenous −OH ligands. Within
the core of these complexes, four Ln<sup>3+</sup>’s are distributed
to the four corners of a perfect square grid while four Ni<sup>2+</sup>’s are projected away from the plane of the Ln<sub>4</sub> unit. Each of the four Ni<sup>2+</sup>’s possesses distorted
octahedral geometry while all of the Ln<sup>3+</sup>’s are
crystallographically equivalent and are present in an elongated square
antiprism geometry. The magnetic properties of compound <b>3</b> are dominated by an easy-plane single-ion anisotropy of the Ni<sup>2+</sup> ions [<i>D</i><sub>Ni</sub> = 6.7(7) K] and dipolar
interactions between Gd<sup>3+</sup> centers. Detailed ac magnetometry
reveals the presence of distinct temperature-dependent out-of-phase
signals for compounds <b>1</b> and <b>2</b>, indicative
of slow magnetic relaxation. Magnetochemical analysis of complex <b>1</b> implies the 3d and the 4f metal ions are engaged in ferromagnetic
interactions with SMM behavior, while dc magnetometry of compound <b>2</b> is suggestive of an antiferromagnetic Ni–Tb spin-exchange
with slow magnetic relaxation due to a field-induced level crossing.
Compound <b>4</b> exhibits an easy-plane single-ion anisotropy
for the Ho<sup>3+</sup> ions and weak interactions between spin centers
Cyclo- and Carbophosphazene-Supported Ligands for the Assembly of Heterometallic (Cu<sup>2+</sup>/Ca<sup>2+</sup>, Cu<sup>2+</sup>/Dy<sup>3+</sup>, Cu<sup>2+</sup>/Tb<sup>3+</sup>) Complexes: Synthesis, Structure, and Magnetism
The carbophosphazene and cyclophosphazene hydrazides,
[{NC(N(CH<sub>3</sub>)<sub>2</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NH<sub>2</sub>}<sub>2</sub>}] (<b>1</b>) and [N<sub>3</sub>P<sub>3</sub>(O<sub>2</sub>C<sub>12</sub>H<sub>8</sub>)<sub>2</sub>{N(CH<sub>3</sub>)NH<sub>2</sub>}<sub>2</sub>] were condensed with <i>o</i>-vanillin
to afford the multisite coordination ligands [{NC(N(CH<sub>3</sub>)<sub>2</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NCH-C<sub>6</sub>H<sub>3</sub>-(<i>o</i>-OH)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}] (<b>2</b>) and [{N<sub>2</sub>P<sub>2</sub>(O<sub>2</sub>C<sub>12</sub>H<sub>8</sub>)<sub>2</sub>}{NP{N(CH<sub>3</sub>)NCH-C <sub>6</sub>H<sub>3</sub>-(<i>o</i>-OH)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}] (<b>3</b>), respectively. These ligands were used for the preparation of heterometallic
complexes [{NC(N(CH<sub>3</sub>)<sub>2</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NCH-C<sub>6</sub>H<sub>3</sub>-(<i>o</i>-O)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}{CuCa(NO<sub>3</sub>)<sub>2</sub>}] (<b>4</b>), [{NC(N(CH<sub>3</sub>)<sub>2</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NCH-C<sub>6</sub>H<sub>3</sub>-(<i>o</i>-O)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}{Cu<sub>2</sub>Ca<sub>2</sub>(NO<sub>3</sub>)<sub>4</sub>}]·4H<sub>2</sub>O (<b>5</b>), [{NC(N(CH<sub>3</sub>)<sub>2</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NCH-C<sub>6</sub>H<sub>3</sub>-(<i>o</i>-O)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}{CuDy(NO<sub>3</sub>)<sub>4</sub>}]·CH<sub>3</sub>COCH<sub>3</sub> (<b>6</b>), [{NP(O<sub>2</sub>C<sub>12</sub>H<sub>8</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NCH-C<sub>6</sub>H<sub>3</sub>-(<i>o</i>-O)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}{CuDy(NO<sub>3</sub>)<sub>3</sub>}] (<b>7</b>), and [{NP(O<sub>2</sub>C<sub>12</sub>H<sub>8</sub>)}<sub>2</sub>{NP{N(CH<sub>3</sub>)NCH-C<sub>6</sub>H<sub>3</sub>-(<i>o</i>-O)(<i>m</i>-OCH<sub>3</sub>)}<sub>2</sub>}{CuTb(NO<sub>3</sub>)<sub>3</sub>}] (<b>8</b>). The
molecular structures of these compounds reveals that the ligands <b>2</b> and <b>3</b> possess dual coordination pockets which
are used to specifically bind the transition metal ion and the alkaline
earth/lanthanide metal ion; the Cu<sup>2+</sup>/Ca<sup>2+</sup>, Cu<sup>2+</sup>/Tb<sup>3+</sup>, and Cu<sup>2+</sup>/Dy<sup>3+</sup> pairs
in these compounds are brought together by phenoxide and methoxy oxygen
atoms. While <b>4</b>, <b>6</b>, <b>7</b>, and <b>8</b> are dinuclear complexes, <b>5</b> is a tetranuclear
complex. Detailed magnetic properties on <b>6</b>–<b>8</b> reveal that these compounds show weak couplings between
the magnetic centers and magnetic anisotropy. However, the ac susceptibility
experiments did not reveal any out of phase signal suggesting that
in these compounds slow relaxation of magnetization is absent above
1.8 K
Mononuclear Lanthanide Complexes: Energy-Barrier Enhancement by Ligand Substitution in Field-Induced Dy<sup>III</sup> SIMs
The sequential reaction of 2-((6-(hydroxymethyl)pyridin-2-yl)-methyleneamino)phenol
(LH<sub>2</sub>), LnCl<sub>3</sub>·6H<sub>2</sub>O, and 1,1,1-trifluoroacetylacetone
(Htfa) in the presence of Et<sub>3</sub>N afforded [Ln(LH) (tfa)<sub>2</sub>] [Ln = Dy<sup>3+</sup> (<b>1</b>), Ln = Tb<sup>3+</sup> (<b>2</b>), and Ln = Gd<sup>3+</sup> (<b>3</b>)], while
under the same reaction conditions, but in the absence of the coligand,
another series of mononuclear complexes, namely, [Ln(LH)<sub>2</sub>]·Cl·2MeOH] [Ln = Dy<sup>3+</sup> (<b>4</b>) and
Tb<sup>3+</sup> (<b>5</b>)] are obtained. Single-crystal X-ray
diffraction analysis revealed that the former set contains a mono-deprotonated
[LH]<sup>−</sup> and two tfa ligands, while the latter set
comprises of two mono-deprotonated [LH]<sup>−</sup> ligands
that are nearly perpendicular to each other at an angle of 86.9°.
Among these complexes, <b>2</b> exhibited a ligand-sensitized
lanthanide-characteristic emission. Analyses of the alternating current
susceptibility measurements reveal the presence of single-molecule
magnet behavior for <b>1</b> and <b>4</b>, in the presence
of direct-current field, with effective energy barriers of 4.6 and
44.4 K, respectively. The enhancement of the effective energy barrier
of the latter can be attributed to the presence of a large energy
gap between the ground and first excited Kramers doublets, triggered
by the change in coordination environments around the lanthanide centers
Novel Chemosensor for the Visual Detection of Copper(II) in Aqueous Solution at the ppm Level
A new water-soluble, multisite-coordinating ligand LH<sub>7</sub> was prepared by the condensation of tris(hydroxymethyl)aminomethane
with 2,6-diformyl-<i>p</i>-cresol. LH<sub>7</sub> is a selective
chemosensor for Cu<sup>2+</sup>, under physiological conditions, with
visual detection limits of 20 ppm (ambient light conditions) and 4
ppm (UV light conditions). LH<sub>7</sub> can also be used in biological
cell lines for the detection of Cu<sup>2+</sup>
Structure–Activity Relationships of Spectinamide Antituberculosis Agents: A Dissection of Ribosomal Inhibition and Native Efflux Avoidance Contributions
Spectinamides are a novel class of antitubercular agents with the potential to treat drug-resistant tuberculosis infections. Their antitubercular activity is derived from both ribosomal affinity and their ability to overcome intrinsic efflux mediated by the Mycobacterium tuberculosis Rv1258c efflux pump. This study explores the structure–activity relationships through analysis of 50 targeted spectinamides. Compounds are evaluated for ribosomal translational inhibition, MIC activity in Rv1258c efflux pump deficient and wild type tuberculosis strains, and efficacy in an acute model of tuberculosis infection. The results of this study show a narrow structure–activity relationship, consistent with a tight ribosome-binding pocket and strict structural requirements to overcome native efflux. Rationalization of ribosomal inhibition data using molecular dynamics simulations showed stable complex formation for halogenated spectinamides consistent with the long post antibiotic effects observed. The lead spectinamides identified in this study demonstrated potent MIC activity against MDR and XDR tuberculosis and had desirable antitubercular class specific features including low protein binding, low microsomal metabolism, no cytotoxicity, and significant reductions in bacterial burdens in the lungs of mice infected with M. tuberculosis. The structure–activity relationships detailed here emphasize the need to examine efflux-mediated resistance in the design of antituberculosis drugs and demonstrate that it is possible to overcome intrinsic efflux with synthetic modification. The ability to understand the structure requirements for this class has produced a variety of new substituted spectinamides, which may provide useful alternative candidates and promote the further development of this class