15 research outputs found
Pulsating Polymer Micelles via ATP-Fueled Dissipative Self-Assembly
Energy
dissipation underlies dynamic behaviors of the life system.
This principle of biology is explicit, but its in vitro mimic is very
challenging. Here we use an energy-dissipative self-assembly pathway
to create a life-like polymer micellar system that can do periodic
and self-adaptive pulsating motion fueled by cell energy currency,
adenosine triphosphate (ATP). Such a micelle expansion–contraction
behavior relies on transient supramolecular interactions between the
micelle and ATP fuel. The micelles capturing ATPs will deviate away
from the thermodynamic equilibrium state, driving a continuous micellar
expansion that temporarily breaks the amphiphilic balance, until a
competing ATP hydrolysis consumes energy to result in an opposing
micellar contraction. As long as ATP energy is supplied to keep the
system in out-of-equilibrium, this reciprocating process can be sustained,
and the ATP level can orchestrate the rhythm and amplitude of nanoparticulate
pulsation. The man-made assemblies provide a model for imitating biologically
time-dependent self-assembly and periodic nanocarriers for programmed
drug delivery
Field-Induced Relaxation of Magnetization in a Three-Dimensional LnMOF with the Second Bridging Ligand Squarate
A three-dimensional
(3D) dysprosiumÂ(III) metal-organic framework
with nicotinate <i>N</i>-oxide (NNO<sup>–</sup>)
and squarate (C<sub>4</sub>O<sub>4</sub><sup>2–</sup>) mixed
bridging ligands, [DyÂ(NNO)Â(C<sub>4</sub>O<sub>4</sub>)Â(H<sub>2</sub>O)]<i><sub>n</sub></i> (<b>1</b>), has been hydrothermally
synthesized. The dysprosiumÂ(III) ions are linked to each other by
the squarate anions to form a unique dysprosiumÂ(III) squarate double-layered
network; the NNO<sup>–</sup> anions then bridge such layers
to complete the 3D framework. Complex <b>1</b> exhibits a two-step
relaxation of magnetization under a dc field of 1000 Oe, with effective
energy barrier values of 8.5 and 14.3 K, respectively
Supplementary document for Modeling off-axis diffraction with adaptive-sampling angular spectrum method - 6442441.pdf
Supplement material with additional results, proof, and derivation
Rigorous and efficient diffraction modeling between arbitrary planes by angular spectrum rearrangement
In computational optics, numerical modeling of diffraction between arbitrary planes offers unparalleled flexibility. However, existing methods suffer from the trade-off between computational accuracy and efficiency. To resolve this dilemma, we present a novel approach that rigorously and efficiently models wave propagation between two arbitrary planes. This is achieved by rearranging the angular spectrum of the source field, coupled with linear algebraic computations. Notably, our method achieves comparable computational efficiency to the control method for both scalar and vectorial diffraction modeling, while eliminating nearly all numerical errors. Furthermore, we selectively merge the angular spectrum to further enhance the efficiency at the expense of precision in a controlled manner. Thereafter, the time consumption is reduced to at most 3% of that before merging
Supplementary document for Investigating deep optics model representation in affecting resolved all-in-focus image quality and depth estimation fidelity - 6046849.pdf
revised supplemental materia
Syntheses, Crystal Structures, and Magnetic Properties of Two <i>p</i>-<i>tert</i>-Butylsulfonylcalix[4]arene Supported Cluster Complexes with a Totally Disordered Ln<sub>4</sub>(OH)<sub>4</sub> Cubane Core
Two new sandwich calix[4]Âarene-supported cluster complexes,
[Ln<sub>4</sub>(OH)<sub>4</sub>Â(TBSOC)<sub>2</sub>Â(H<sub>2</sub>O)<sub>4</sub>Â(CH<sub>3</sub>OH)<sub>4</sub>]·4H<sub>2</sub>O (H<sub>4</sub>TBSOC = <i>p</i>-<i>tert</i>-butylsulfonylcalixÂ[4]Âarene; Ln = Dy, <b>1</b>; Ln = Ho, <b>2</b>), have been prepared and characterized. An X-ray crystallographic
study reveals that both complexes contain a holistically disordered
[Ln<sub>4</sub>(OH)<sub>4</sub>]<sup>8+</sup> cubane cluster core,
which is sandwiched between two antiparallel calixarene macrocycles.
Magnetic investigations indicate that complex <b>1</b> displays
slow magnetization relaxation typical for single-molecule magnets
in the absence of a static applied dc field, with the Δ<i><i>E</i>/k</i><sub>B</sub> parameter of 22.9 K, the
largest value for the calixarene-supported pure 4f single-molecule
magnets so far, whereas complex <b>2</b> does not show any relaxation
of the magnetization above 2 K
Arraying Octahedral {Cr<sub>2</sub>Dy<sub>4</sub>} Units into 3D Single-Molecule-Magnet-Like Inorganic Compounds with Sulfate Bridges
Two novel 3D pure
inorganic compounds based on [Cr<sub>2</sub>Dy<sub>4</sub>(ÎĽ<sub>4</sub>-O)<sub>2</sub>(ÎĽ<sub>3</sub>-OH)<sub>4</sub>]<sup>10+</sup> cluster units and sulfate anions are presented. Both complexes exhibit
single-molecule-magnet (SMM)-like behavior. Permutation of the magnetic
moment direction among SMM-like cluster units has a significant effect
on the performance of molecular nanomagnets, and directional consistency
shows obvious advantages
Syntheses, Crystal Structures, and Magnetic Properties of Two <i>p</i>-<i>tert</i>-Butylsulfonylcalix[4]arene Supported Cluster Complexes with a Totally Disordered Ln<sub>4</sub>(OH)<sub>4</sub> Cubane Core
Two new sandwich calix[4]Âarene-supported cluster complexes,
[Ln<sub>4</sub>(OH)<sub>4</sub>Â(TBSOC)<sub>2</sub>Â(H<sub>2</sub>O)<sub>4</sub>Â(CH<sub>3</sub>OH)<sub>4</sub>]·4H<sub>2</sub>O (H<sub>4</sub>TBSOC = <i>p</i>-<i>tert</i>-butylsulfonylcalixÂ[4]Âarene; Ln = Dy, <b>1</b>; Ln = Ho, <b>2</b>), have been prepared and characterized. An X-ray crystallographic
study reveals that both complexes contain a holistically disordered
[Ln<sub>4</sub>(OH)<sub>4</sub>]<sup>8+</sup> cubane cluster core,
which is sandwiched between two antiparallel calixarene macrocycles.
Magnetic investigations indicate that complex <b>1</b> displays
slow magnetization relaxation typical for single-molecule magnets
in the absence of a static applied dc field, with the Δ<i><i>E</i>/k</i><sub>B</sub> parameter of 22.9 K, the
largest value for the calixarene-supported pure 4f single-molecule
magnets so far, whereas complex <b>2</b> does not show any relaxation
of the magnetization above 2 K
Soluble Silver Acetylide for the Construction and Structural Conversion of All-Alkynyl-Stabilized High-Nuclearity Homoleptic Silver Clusters
Silver
acetylide complex [AgÂ(ArCî—ĽC)]<sub><i>n</i></sub> (Ar
= 3,5-di-<i>tert</i>-butylphenyl) with unprecedented
high solubility in common organic solvents has been designed and synthesized.
The high solubility is due to two bulky <i>tert</i>-butyl
substituents on the phenyl ring. This feature is significant to construct
and isolate single crystals of all-alkynyl-stabilized silver clusters,
which are crucial to investigate the intrinsic binding interaction
and coordination modes between AgÂ(I) and ethynide ligands. Crystallization
of [AgÂ(ArCî—ĽC)]<sub><i>n</i></sub> under various conditions
resulted in three high-nuclearity homoleptic silver acetylide clusters,
namely, [Ag<sub>21</sub>(ArCî—ĽC)<sub>20</sub>]Â(OH) (<b>1</b>), [Ag<sub>16</sub>(ArCî—ĽC)<sub>16</sub>] (<b>2</b>),
and [Ag<sub>15</sub>(ArCî—ĽC)<sub>15</sub>] (<b>3</b>).
Complex <b>1</b> has a [Ag<sub>21</sub>] cluster protected by
twenty 3,5-di-<i>tert</i>-butyl-phenylethynide ligands.
Complexes <b>2</b> and <b>3</b> have neutral [Ag<sub>16</sub>] and [Ag<sub>15</sub>] clusters, respectively. In addition to these
homoleptic silver clusters, two new silver acetylides [Ag<sub>20</sub>(ArCî—ĽC)<sub>16</sub>(CH<sub>3</sub>COO)<sub>4</sub>] (<b>4</b>) and [Ag<sub>22</sub>(ArCî—ĽC)<sub>16</sub>(NO<sub>3</sub>)<sub>4</sub>(CH<sub>3</sub>CH<sub>2</sub>OH)<sub>4</sub>]Â(OH)<sub>2</sub> (<b>5</b>) were synthesized. The acetate and nitrate
anions in these structures are more like counterions instead of acting
as critical building blocks or templates for cluster assembly. These
results illustrated the significance of 3,5-di-<i>tert</i>-butyl-phenylethynide ligands in the construction and stabilization
of high-nuclearity silver clusters. Analysis of structures of <b>1</b>–<b>5</b> revealed several novel coordination
modes between AgÂ(I) and ethynide ligands, which contributed considerably
to our knowledge of AgÂ(I)–ethynide binding interactions
Chloroyttrium 2‑(1-(Arylimino)alkyl)quinolin-8-olate Complexes: Synthesis, Characterization, and Catalysis of the Ring-Opening Polymerization of ε‑Caprolactone
Stoichiometric reactions of YCl<sub>3</sub>(THF)<sub>3</sub> with
potassium 2-((arylimino)Âmethyl)Âquinolin-8-olates or 2-(1-(arylimino)Âethyl)Âquinolin-8-olates
in THF solution gave the mononuclear LYCl<sub>2</sub>(DMSO)<sub>2</sub> complexes <b>1</b>–<b>5</b> in the presence of
DMSO and a representative dinuclear complex <b>6</b> in the
absence of DMSO. All yttrium complexes were fully characterized by
NMR measurements and elemental analysis, and the crystal structures
of complexes <b>1</b> and <b>4</b>–<b>6</b> were determined by single-crystal X-ray diffraction. The structures
indicate coordination number seven around the yttrium center and pentagonal
bipyramidal geometries. The complexes all feature diapical YCl<sub>2</sub> moieties and one tridentate organic ligand in the equatorial
plane. Upon reaction of the yttrium precatalysts <b>1</b>–<b>6</b> with LiCH<sub>2</sub>SiÂ(CH<sub>3</sub>)<sub>3</sub> alone
or with LiCH<sub>2</sub>SiÂ(CH<sub>3</sub>)<sub>3</sub> together with
BnOH, the ring-opening polymerization (ROP) of ε-caprolactone
(ε-CL) occurred with high efficiency. Depending on conditions,
the ROP of ε-CL produced polycaprolactone with narrow molecular
distribution and in a living manner. Theoretical studies of the chlorine/CH<sub>2</sub>SiMe<sub>3</sub> and Me<sub>3</sub>SiCH<sub>2</sub>/BnO ligand
exchange reactions suggest that the replacement of the apical ligands
can proceed without significantly affecting the equatorial ligands.
These results suggest that one of the apical Y–CH<sub>2</sub>SiMe<sub>3</sub> bonds within the LYÂ(CH<sub>2</sub>SiMe<sub>3</sub>)<sub>2</sub> intermediate catalyzes the polymerization in the BnOH-free
process. Most polymers generated by BnOH-assisted catalysis possess <i>M</i><sub>n</sub> values that are similar to <i>M</i><sub>n,cal</sub> values based on Y–OBn, suggesting that one
apical Y–OBn bond of the diapical LYÂ(OBn)Â(CH<sub>2</sub>SiMe<sub>3</sub>) intermediate catalyzes most or all of the ring polymerization
of ε-CL