11 research outputs found
Two Zinc(II) Complexes with 1D Chain and 2D Layer Directed by Competitive Coordination of the Mixed Ligands: Syntheses, Crystal Structures, and Fluorescent Properties
<p>Two new competitive coordination-directed zinc(II) complexes, [Zn<sub>2</sub>(bpp)<sub>2</sub>(na)<sub>4</sub>]<i><sub>n</sub></i> (<b>1</b>) and [Zn(bpp)<sub>2</sub>(nas)<sub>2</sub>]<i><sub>n</sub></i> (<b>2</b>) (bpp = 1,3-bi(4-pyridyl)propane, na<sup>−</sup> = 1-naphthoate, and nas<sup>−</sup> = 2-aminonaphthalene-1-sulfonate), were hydrothermally synthesized by varying carboxylate- or sulfonate-containing coligands. Structural analyses reveal that complex <b>1</b> modified by terminal na<sup>−</sup> spacers possesses a bent one-dimensional chain bridged by ditopic bpp linkers. By contrast, complex <b>2</b> with two monodentate nas<sup>−</sup> ligands exhibits a two-dimensional layered structure extended by four equatorial bpp connectors. Obviously, the increase on the dimensionality of <b>2</b> than <b>1</b> is significantly resulting from the competitive coordination of the two mixed ligands with differently tunable binding groups to variable metal polyhedra. In addition, both complexes with analogously high thermal stability display strong fluorescent emissions at room temperature resulting from the ligand-to-metal or intraligand charge-transfer, suggesting their hopeful applications as efficient fluorescent materials.</p
Three-Dimensional Hierarchical Nickel Cobalt Phosphide Nanoflowers as an Efficient Electrocatalyst for the Hydrogen Evolution Reaction under Both Acidic and Alkaline Conditions
The
sustainable hydrogen fuel from water electrolysis demands the development
of efficient and robust non-noble electrocatalysts for the hydrogen
evolution reaction (HER). Tuning the morphology and chemical composition
is paramount to constructing electrocatalysts with superior activity
and stability. In this work, novel ternary nickel-doped cobalt phosphide
(Ni–Co–P) nanoflowers assembled by porous and unltrathin
nanosheets were first prepared by a facile solvothermal reaction following
a phosphidation procedure. The Ni–Co–P nanoflowers exhibited
remarkable electrocatalytic HER performance, exhibiting overpotentials
of as low as 83 and 92 mV at 10 mA cm<sup>–2</sup> and small
Tafel slopes of 46.6 and 49.6 mV dec<sup>–1</sup> under1 M
KOH and 0.5 M H<sub>2</sub>SO<sub>4</sub> conditions, respectively,
which was one of the most active earth-abundant electrocatalysts.
Additionally, the electrocatalysts exhibited high durability for HER
under both alkaline and acidic conditions. Various techniques further
demonstrated that the superior activity of Ni–Co–P nanoflowers
was attributed to the unique 3D hierarchical morphology and the modified
electron structure due to Ni incorporation. The superior activity
and stability of novel Ni–Co–P nanoflowers hold promising
potential for applications in the production of hydrogen fuel from
water splitting
Diverse Self-Assembly from Predesigned Conformationally Flexible Pentanuclear Clusters Observed in a Ternary Copper(II)–Triazolate–Sulfoisophthalate System: Synthesis, Structure, and Magnetism
Self-assembly from the predesigned
Cu<sup>II</sup><sub>5</sub> secondary building unit (SBU) in the ternary
Cu<sup>II</sup>–triazolate–sulfoisophthalate system
generates three interesting magnetic samples: an open pillared-layer
framework with nanosized Cu<sup>II</sup><sub>30</sub> metallamacrocycle-based
sublayer (<b>1</b>), a (3,6)-connected 2-fold interpenetrating
network consisting of alternating Cu<sup>II</sup><sub>5</sub> and
Cu<sup>II</sup><sub>1</sub> cores (<b>2</b>), and a (4,8)-connected
architecture constructed from centrosymmetric Cu<sup>II</sup><sub>7</sub> clusters and four-branched 5-sulfoisophthalate (sip<sup>3–</sup>) connectors (<b>3</b>). These various structures significantly
result from the variable connectivity and the slight expansion of
the predetermined conformationally flexible Cu<sup>II</sup><sub>5</sub> SBUs. Furthermore, these intriguing structural motifs in <b>1</b>–<b>3</b> essentially induce different magnetic phenomena.
A field-dependent metamagnetic transition from antiferromagnetic ordering
to weak ferromagnetism is observed in the frustrated Cu<sup>II</sup><sub>30</sub>-based sublayer of <b>1</b>. The paramagnetic
Cu<sup>II</sup><sub>1</sub> core in <b>2</b> virtually contributes
to an <i>S</i> = <sup>1</sup>/<sub>2</sub> spin ground state
due to the completely compensated magnetic moment in the 1,2,3-triazolate
(ta<sup>–</sup>)-bridged Cu<sup>II</sup><sub>5</sub> cluster
containing ribbon. In contrast, strong antiferromagnetic interactions
in the locally centrosymmetric Cu<sup>II</sup><sub>7</sub> cluster
lead to an overall <i>S</i> = <sup>1</sup>/<sub>2</sub> spin
ground state of <b>3</b>. Thus, the SBU-derived self-assembly
strategy provides important hints for polymetallic cluster based high-dimensional
magnetic materials, which also brings a new vision for the design
and construction of novel functional materials
Diverse Self-Assembly from Predesigned Conformationally Flexible Pentanuclear Clusters Observed in a Ternary Copper(II)–Triazolate–Sulfoisophthalate System: Synthesis, Structure, and Magnetism
Self-assembly from the predesigned
Cu<sup>II</sup><sub>5</sub> secondary building unit (SBU) in the ternary
Cu<sup>II</sup>–triazolate–sulfoisophthalate system
generates three interesting magnetic samples: an open pillared-layer
framework with nanosized Cu<sup>II</sup><sub>30</sub> metallamacrocycle-based
sublayer (<b>1</b>), a (3,6)-connected 2-fold interpenetrating
network consisting of alternating Cu<sup>II</sup><sub>5</sub> and
Cu<sup>II</sup><sub>1</sub> cores (<b>2</b>), and a (4,8)-connected
architecture constructed from centrosymmetric Cu<sup>II</sup><sub>7</sub> clusters and four-branched 5-sulfoisophthalate (sip<sup>3–</sup>) connectors (<b>3</b>). These various structures significantly
result from the variable connectivity and the slight expansion of
the predetermined conformationally flexible Cu<sup>II</sup><sub>5</sub> SBUs. Furthermore, these intriguing structural motifs in <b>1</b>–<b>3</b> essentially induce different magnetic phenomena.
A field-dependent metamagnetic transition from antiferromagnetic ordering
to weak ferromagnetism is observed in the frustrated Cu<sup>II</sup><sub>30</sub>-based sublayer of <b>1</b>. The paramagnetic
Cu<sup>II</sup><sub>1</sub> core in <b>2</b> virtually contributes
to an <i>S</i> = <sup>1</sup>/<sub>2</sub> spin ground state
due to the completely compensated magnetic moment in the 1,2,3-triazolate
(ta<sup>–</sup>)-bridged Cu<sup>II</sup><sub>5</sub> cluster
containing ribbon. In contrast, strong antiferromagnetic interactions
in the locally centrosymmetric Cu<sup>II</sup><sub>7</sub> cluster
lead to an overall <i>S</i> = <sup>1</sup>/<sub>2</sub> spin
ground state of <b>3</b>. Thus, the SBU-derived self-assembly
strategy provides important hints for polymetallic cluster based high-dimensional
magnetic materials, which also brings a new vision for the design
and construction of novel functional materials
Structural Transformation from a Discrete Cu<sup>II</sup><sub>4</sub> Cluster to Two Extended Cu<sup>II</sup><sub>4</sub> + Cu<sup>II</sup><sub>1</sub> Chain-Based Three-Dimensional Frameworks by Changing the Spacer Functionality: Synthesis, Crystal Structures, and Magnetic Properties
Three unique [Cu<sub>4</sub>(μ<sub>3</sub>-OH)<sub>2</sub>]<sup>6+</sup> core-based magnetic complexes, [Cu<sub>4</sub>(amtrz)<sub>2</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(nb)<sub>6</sub>]·2H<sub>2</sub>O (<b>1</b>), {[Cu<sub>5</sub>(H<sub>2</sub>O)<sub>6</sub>(trz)<sub>2</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(btc)<sub>2</sub>]·0.6H<sub>2</sub>O}<sub><i>n</i></sub> (<b>2</b>), and {[Cu<sub>5</sub>(H<sub>2</sub>O)<sub>2</sub>(Htrz)<sub>2</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(btec)<sub>2</sub>]·0.125H<sub>2</sub>O}<sub><i>n</i></sub> (<b>3</b>) (amtrz =
4-amino-1,2,4-triazole, Htrz = 1,2,4-triazole, Hnb = 4-nitrobenzoic
acid, H<sub>3</sub>btc = 1,2,3-benzenetricarboxylic acid, and H<sub>4</sub>btec = 1,2,4,5-benzenetetracarboxylic acid), were synthesized
by varying the spacer functionality of the mixed ligands. Significantly
resulting from the cooperative cocoordination of the metal ions with
polytopic triazolyl and carboxylate groups, a structural transformation
from a discrete Cu<sup>II</sup><sub>4</sub> cluster for <b>1</b> to two alternate Cu<sup>II</sup><sub>4</sub> + Cu<sup>II</sup><sub>1</sub> chain-based three-dimensional frameworks for <b>2</b> and <b>3</b> was achieved. Moreover, the connectivity manner
of the structural subunits in <b>2</b> and <b>3</b> depends
strongly on the number and position of the carboxylate group attached
on the phenyl backbone. The nearest-neighbor interactions within the
Cu<sup>II</sup><sub>4</sub> cluster and between Cu<sup>II</sup><sub>4</sub> cluster and Cu<sup>II</sup><sub>1</sub> core mediated by
the mixed short bridges were quantitatively calculated and compared
based on the established magneto-structural relationships. Strong
antiferromagnetic coupling interactions up to −206(4) cm<sup>–1</sup> were observed in the isolated Cu<sup>II</sup><sub>4</sub> cluster due to the favorable spatial orientation of the mixed
multiple heterobridges toward the spin carriers
Diverse Self-Assembly from Predesigned Conformationally Flexible Pentanuclear Clusters Observed in a Ternary Copper(II)–Triazolate–Sulfoisophthalate System: Synthesis, Structure, and Magnetism
Self-assembly from the predesigned
Cu<sup>II</sup><sub>5</sub> secondary building unit (SBU) in the ternary
Cu<sup>II</sup>–triazolate–sulfoisophthalate system
generates three interesting magnetic samples: an open pillared-layer
framework with nanosized Cu<sup>II</sup><sub>30</sub> metallamacrocycle-based
sublayer (<b>1</b>), a (3,6)-connected 2-fold interpenetrating
network consisting of alternating Cu<sup>II</sup><sub>5</sub> and
Cu<sup>II</sup><sub>1</sub> cores (<b>2</b>), and a (4,8)-connected
architecture constructed from centrosymmetric Cu<sup>II</sup><sub>7</sub> clusters and four-branched 5-sulfoisophthalate (sip<sup>3–</sup>) connectors (<b>3</b>). These various structures significantly
result from the variable connectivity and the slight expansion of
the predetermined conformationally flexible Cu<sup>II</sup><sub>5</sub> SBUs. Furthermore, these intriguing structural motifs in <b>1</b>–<b>3</b> essentially induce different magnetic phenomena.
A field-dependent metamagnetic transition from antiferromagnetic ordering
to weak ferromagnetism is observed in the frustrated Cu<sup>II</sup><sub>30</sub>-based sublayer of <b>1</b>. The paramagnetic
Cu<sup>II</sup><sub>1</sub> core in <b>2</b> virtually contributes
to an <i>S</i> = <sup>1</sup>/<sub>2</sub> spin ground state
due to the completely compensated magnetic moment in the 1,2,3-triazolate
(ta<sup>–</sup>)-bridged Cu<sup>II</sup><sub>5</sub> cluster
containing ribbon. In contrast, strong antiferromagnetic interactions
in the locally centrosymmetric Cu<sup>II</sup><sub>7</sub> cluster
lead to an overall <i>S</i> = <sup>1</sup>/<sub>2</sub> spin
ground state of <b>3</b>. Thus, the SBU-derived self-assembly
strategy provides important hints for polymetallic cluster based high-dimensional
magnetic materials, which also brings a new vision for the design
and construction of novel functional materials
Molecular Binding Behaviors of Sulfonated Calixarenes with Phenanthroline-diium in Aqueous Solution and Solid State: Cavity Size Governing Capsule Formation
The
molecular binding behaviors of <i>p</i>-sulfonatocalixÂ[4]Âarene
(SC4A), <i>p</i>-sulfonatocalixÂ[5]Âarene (SC5A),
and <i>p</i>-sulfonatothiacalixÂ[4]Âarene (STC4A)
with 5,6-dihydropyrazionÂ[1,2,3,4-<i>lmn</i>]Â[1,10]Âphenanthroline-4,7-diium
(DP<sup>2+</sup>) were systematically investigated by crystallography,
NMR spectroscopy, and microcalorimetry at pH 1–2. The obtained
results showed that, in both aqueous solution and the solid state,
DP<sup>2+</sup> was immersed into the cavity of the sulfonated calixarene
host in a slantwise degree with the aromatic moiety being included
first. The different slantwise degree of the guest in the host cavity
determined whether the host–guest capsule could be formed in
the solid state. Furthermore, all three sulfonated calixarene hosts
showed high affinities with DP<sup>2+</sup> in the magnitude of 10<sup>5</sup>–10<sup>6</sup> M<sup>–1</sup> in aqueous solution,
and the binding modes for host–guest complexation were explained
from a thermodynamic viewpoint
Three Isostructural One-Dimensional Ln<sup>III</sup> Chains with Distorted Cubane Motifs Showing Dual Fluorescence and Slow Magnetic Relaxation/Magnetocaloric Effect
Three
new homometallic lanthanide complexes with mixed carboxylate-modified
rigid ligands, [LnÂ(μ<sub>3</sub>-OH)Â(na)Â(pyzc)]<sub><i>n</i></sub> (na<sup>–</sup> = 1-naphtholate, pyzc<sup>–</sup> = 2-pyrazinecarboxylate, Ln = Dy (<b>1</b>),
Yb (<b>2</b>), and Gd (<b>3</b>)), were solvothermally
synthesized, and their structures and magnetic as well as photophysical
properties were completely investigated. Complexes <b>1</b>–<b>3</b> are crystallographically isostructural, exhibiting linear
chains with four bidentate bridging μ-COO<sup>–</sup> moieties encapsulated cubic {Ln<sub>4</sub>(μ<sub>3</sub>-OH)<sub>4</sub>}<sup>8+</sup> clusters repeatedly extended by 4-fold chelating-bridging-pyzc<sup>–</sup> connectors. Magnetically, the former two complexes
with highly anisotropic Dy<sup>III</sup> and weak anisotropic Yb<sup>III</sup> ions in the distorted NO<sub>7</sub> triangular dodecahedron
coordination environment display field-induced slow relaxation of
magnetization. Fitting the dynamic magnetic data to the Arrhenius
law gives energy barrier Δ<i>E</i>/<i>k</i><sub>B</sub> = 39.6 K and pre-exponential factor τ<sub>o</sub> = 1.52 × 10<sup>–8</sup> s for <b>1</b> and Δ<i>E</i>/<i>k</i><sub>B</sub> = 14.1 K and τ<sub>o</sub> = 2.13 × 10<sup>–7</sup> s for <b>2</b>. By contrast, complex <b>3</b> with isotropic Gd<sup>III</sup> ion and weak intracluster antiferromagnetic coupling shows a significant
cryogenic magnetocaloric effect, with a maximum −Δ<i>S</i><sub>m</sub> value of 30.0 J kg<sup>–1</sup> K<sup>–1</sup> at 2.5 K and 70 kOe. Additionally, the chromophoric
na<sup>–</sup> and pyzc<sup>–</sup> ligands can serve
as antenna groups, selectively sensitizing the Dy<sup>III</sup>- and
Yb<sup>III</sup>-based luminescence of <b>1</b> and <b>2</b> in the UV–visible region by an intramolecular energy transfer
process. Thus, complexes <b>1</b>–<b>3</b>, incorporating
field-induced slow magnetic magnetization and interesting luminescence
together, can be used as composite magneto-optical materials. More
importantly, these interesting results further demonstrate that the
mixed-ligand system with rigid carboxylate-functionalized chromophores
can be excellent candidates for the preparations of new bifunctional
magneto-optical materials
Magnetic Relaxation Dynamics of a Centrosymmetric <b>Dy<sub>2</sub></b> Single-Molecule Magnet Triggered by Magnetic-Site Dilution and External Magnetic Field
A centrosymmetric <b>Dy</b><sub><b>2</b></sub> single-molecule magnet (SMM) and its doped
diamagnetic yttrium analogues, <b>Dy</b><sub><b>0.19</b></sub><b>Y</b><sub><b>1.81</b></sub> and <b>Dy</b><sub><b>0.10</b></sub><b>Y</b><sub><b>1.90</b></sub>, were solvothermally synthesized to investigate the effects of intramolecular
exchange coupling and quantum tunneling of magnetization (QTM) on
the magnetic relaxation dynamics. Constructed from two hula-hoop-like
Dy<sup>III</sup> ions and a pair of phenoxido groups, the antiferromagnetically
coupled <b>Dy</b><sub><b>2</b></sub> exhibits a thermal-activated
zero-field effective energy barrier (<i>U</i><sub>eff</sub>) of 277.7 K and negligible hysteresis loop at 2.0 K. The doping
of a diamagnetic Y<sup>III</sup> matrix with 90.5% and 95.0% molar
ratios reveals the single-ion origin of the Orbach channel, increases
the relaxation time by partially quenching the QTM process, and induces
an open hysteresis loop until 5.0 K. In contrast, an optimal dc field
of 1.0 kOe improves the barrier height up to 290.1 K through complete
elimination of the QTM and delays the relaxation time of the direct
relaxation pathway. More interestingly, the collaborative dual effects
of magnetic-site dilution and external magnetic field make the effective
energy barrier and relaxation time increase 8.1% and 49 times, respectively.
Thus, the overall magnetization dynamics of the <b>Dy</b><sub><b>2</b></sub> system systematically elaborate the inherent
interplay of the QTM and Orbach processes on the effective energy
barrier, highlighting the vital role of the relaxation time on the
coercive hysteresis loop
Two 3-Amino-1,2,4-triazole-based Manganese(II) Complexes Incorporated With Different Dicarboxylate Coligands: Synthesis, Structure, and Magnetism
<div><p>Two 3-amino-1,2,4-triazole (Hatz)-based magnetic complexes, {[Mn<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Hatz)<sub>2</sub>(sip)<sub>2</sub>]·2H<sub>2</sub>O}<i><sub>n</sub></i> (<b>1</b>) and {[Mn(H<sub>2</sub>O)<sub>3</sub>(Hatz)(bda)]·H<sub>2</sub>O}<i><sub>n</sub></i> (<b>2</b>) (sip<sup>3−</sup> = 5-sulfoisophthalate and bda<sup>2−</sup> = <i>trans</i>-butenedioate), were respectively prepared by varying dicarboxylate-containing coligands, and were structurally and magnetically characterized. Structural determinations reveal that <b>1</b> exhibits a two-dimensional layered structure with linear {Mn<sub>3</sub>(μ-N1,N2-Hatz)<sub>2</sub>}<sup>6+</sup> subunits extended by tritopic sip<sup>3−</sup> connectors. By contrast, <b>2</b> is an infinite <i>zigzag</i> chain constructed from octahedral Mn(II) ions and μ-N1,N4-Hatz linkers. Magnetically, typically antiferromagnetic interaction observed in the local Mn<sup>II</sup><sub>3</sub> subunit of <b>1</b> mediated by mixed μ-<i>syn, syn</i>-COO<sup>−</sup> and μ-N1,N2-Hatz heterobridges is slightly stronger than that of <b>2</b> transmitted by single μ-N1,N4-Hatz mediator.</p></div