25 research outputs found
The First Uranyl Arsonates Featuring Heterometallic Cation–Cation Interactions with U<sup>VI</sup>O–Zn<sup>II</sup> Bonding
Two new uranyl arsonates, ZnÂ(UO<sub>2</sub>)Â(PhAsO<sub>3</sub>)<sub>2</sub>L·H<sub>2</sub>O [L = 1,10-phenanthroline
(<b>1</b>) and 2,2′-bipyridine (<b>2</b>)], have
been synthesized
by hydrothermal reactions of phenylarsonic acid, L, and ZnUO<sub>2</sub>(OAc)<sub>4</sub>·7H<sub>2</sub>O. Single-crystal X-ray analyses
demonstrate that these two compounds are isostructural and exhibit
one-dimensional chains in which U<sup>VI</sup> and Zn<sup>II</sup> cations are directly connected by the <i>yl</i> oxygen
atoms and additionally bridged by arsonate groups. Both compounds
represent the first examples of uranyl arsonates with heterometallic
cation–cation interactions
Weak Bimetal Coupling-Assisted MN<sub>4</sub> Catalyst for Enhanced Carbon Dioxide Reduction Reaction
The
design of multimetal catalysts holds immense significance for
efficient CO2 capture and its conversion into economically
valuable chemicals. Herein, heterobimetallic catalysts (MiMo)L were exploited for the CO2 reduction reactions
(CO2RR) using relativistic density functional theory (DFT).
The octadentate Pacman-like polypyrrolic ligand (H4L) accommodates
two metal ions (Mo, W, Nd, and U) inside (Mi) and outside
(Mo) its month, rendering a weak bimetal coupling-assisted
MN4 catalytically active site. Adsorption reactions have
access to energetically stable coordination modes of –OCO, –OOC, and –(OCO)2, where the donor atom(s) are marked in bold. Among
all of the species, (UiMoo)L releases the most
energy. Along CO2RR, it favors to produce CO. The high-efficiency
CO2 reduction is attributed to the size matching of U with
the ligand mouth and the effective manipulation of the electron density
of both ligand and bimetals. The mechanism in which heterobimetals
synergetically capture and reduce CO2 has been postulated.
This establishes a reference in elaborating on the complicated heterogeneous
catalysis
Highly Valence-Diversified Binuclear Uranium Complexes of a Schiff-Base Polypyrrolic Macrocycle: Prediction of Unusual Structures, Electronic Properties, and Formation Reactions
On the basis of relativistic density
functional theory calculations, homo- and heterovalent binuclear uranium
complexes of a polypyrrolic macrocycle in a U–O–U bridging
fashion have been investigated. These complexes show a variety of
oxidation states for uranium ranging from III to VI, which have been
confirmed by the calculated electron-spin density on each metal center.
An equatorially 5-fold uranyl coordination mode is suitable for hexavalent
uranium complexes, while silylation of the uranyl oxo is favored by
pentavalent uranium. Uranyl oxo ligands are not required anymore for
the coordination environment of tetra- and trivalent uranium because
of their replacement by strong donors such as tetrahydrofuran and
iodine. Optimization of binuclear U<sup>VI</sup>–U<sup>III</sup> complexes with various coordinating modes of U<sup>III</sup>, donor
numbers, and donor types reveals that 0.5–1.0 electron has
been transferred from U<sup>III</sup> to U<sup>VI</sup>. Consequently,
U<sup>V</sup>–U<sup>IV</sup> complexes are more favorable.
Electronic structures and formation reactions of several representative
uranium complexes were calculated. For example, a 5f-based σÂ(U–U)
bonding orbital is found in the diuraniumÂ(IV) complex, rationalizing
the fact that it shows the shortest U–U distance (3.82 Å)
among the studied binuclear complexes
Interfacial Interaction of Titania Nanoparticles and Ligated Uranyl Species: A Relativistic DFT Investigation
To
understand interfacial behavior of actinides adsorbed onto mineral
surfaces and unravel their structure–property relationship,
the structures, electronic properties, and energetics of various ligated
uranyl species adsorbed onto TiO<sub>2</sub> surface nanoparticle
clusters (SNCs) were examined using relativistic density functional
theory. Rutile (110) and anatase (101) titania surfaces, experimentally
known to be stable, were fully optimized. For the former, models studied
include clean and water-free Ti<sub>27</sub>O<sub>64</sub>H<sub>20</sub> (<b>dry</b>), partially hydrated (Ti<sub>27</sub>O<sub>64</sub>H<sub>20</sub>)Â(H<sub>2</sub>O)<sub>8</sub> (<b>sol</b>) and
proton-saturated [(Ti<sub>27</sub>O<sub>64</sub>H<sub>20</sub>)Â(H<sub>2</sub>O)<sub>8</sub>(H)<sub>2</sub>]<sup>2+</sup> (<b>sat</b>), while defect-free and defected anatase SNCs involving more than
38 TiO<sub>2</sub> units were considered. The aquouranyl sorption
onto rutile SNCs is energetically preferred, with interaction energies
of −8.54, −10.36, and −2.39 eV, respectively.
Energy decomposition demonstrates that the sorption is dominated by
orbital attractive interactions and modified by steric effects. Greater
hydrogen-bonding involvement leads to increased orbital interactions
(i.e., more negative energy) from <b>dry</b> to <b>sol/sat</b> complexes, while much larger steric interaction in the <b>sat</b> complex significantly reduces the sorption interaction (i.e., more
positive energy). For <b>dry</b> SNC, adsorbates were varied
from aquo to aquo-carbonato, to carbonato, to hydroxo uranyl species.
Longer U–O<sub>surf</sub>/U–Ti distances and more positive
sorption energies were calculated upon introducing carbonato and hydroxo
ligands, indicative of weaker uranyl sorption onto the substrate.
This is consistent with experimental observations that the uranyl
sorption rate decreases upon raising solution pH value or adding carbon
dioxide. Anatase SNCs adsorbing aquouranyl are even more exothermic,
because more bonds are formed than in the case of rutile. Moreover,
the anatase sorption can be tuned by surface defects as well as its
Ti and O stoichiometry. All the aquouranyl–SNC complexes show
similar character of molecular orbitals and energetic order although
differing in highest occupied molecular orbital (HOMO)–lowest
unoccupied molecular orbital (LUMO) gaps and orbital energy levels,
but changes can be accomplished by adding carbonato and hydroxo ligands
The First Uranyl Arsonates Featuring Heterometallic Cation–Cation Interactions with U<sup>VI</sup>O–Zn<sup>II</sup> Bonding
Two new uranyl arsonates, ZnÂ(UO<sub>2</sub>)Â(PhAsO<sub>3</sub>)<sub>2</sub>L·H<sub>2</sub>O [L = 1,10-phenanthroline
(<b>1</b>) and 2,2′-bipyridine (<b>2</b>)], have
been synthesized
by hydrothermal reactions of phenylarsonic acid, L, and ZnUO<sub>2</sub>(OAc)<sub>4</sub>·7H<sub>2</sub>O. Single-crystal X-ray analyses
demonstrate that these two compounds are isostructural and exhibit
one-dimensional chains in which U<sup>VI</sup> and Zn<sup>II</sup> cations are directly connected by the <i>yl</i> oxygen
atoms and additionally bridged by arsonate groups. Both compounds
represent the first examples of uranyl arsonates with heterometallic
cation–cation interactions
Electron-Transfer-Enhanced Cation–Cation Interactions in Homo- and Heterobimetallic Actinide Complexes: A Relativistic Density Functional Theory Study
To provide deep insight into cation–cation
interactions (CCIs) involving hexavalent actinyl species that are
major components in spent nuclear fuel and pose important implications
for the effective removal of radiotoxic pollutants in the environment,
a series of homo- and heterobimetallic actinide complexes supported
by cyclopentadienyl (Cp) and polypyrrolic macrocycle (H<sub>4</sub>L) ligands were systematically investigated using relativistic density
functional theory. The metal sort in both parts of (THF)Â(H<sub>2</sub>L)Â(OAn<sup>VI</sup>O) and (An′)<sup>III</sup>Cp<sub>3</sub> from U to Np to Pu, as well as the substituent bonding to Cp from
electron-donating Me to H to electron-withdrawing Cl, SiH<sub>3</sub>, and SiMe<sub>3</sub>, was changed. Over 0.70 electrons are unraveled
to transfer from the electron-rich U<sup>III</sup> to the electron-deficient
An<sup>VI</sup> of the actinyl moiety, leading to a more stable An<sup>V</sup>–U<sup>IV</sup> isomer; in contrast, uranylneptunium
and uranylplutonium complexes behave as electron-resonance structures
between VI–III and V–IV. These were further corroborated
by geometrical and electronic structures. The energies of CCIs (i.e.,
O<sub>exo</sub>–An′ bonds) were calculated to be −19.6
to −41.2 kcal/mol, affording those of OUO–Np (−23.9
kcal/mol) and OUO–Pu (−19.6 kcal/mol) with less electron
transfer (ET) right at the low limit. Topological analyses of the
electron density at the O<sub>exo</sub>–An′ bond critical
points demonstrate that the CCIs are ET or dative bonds in nature.
A positive correlation has been built between the CCIs’ strength
and corresponding ET amount. It is concluded that the CCIs of O<sub>exo</sub>–An′ are driven by the electrostatic attraction
between the actinyl oxo atom (negative) and the actinide ion (positive)
and enhanced by their ET. Finally, experimental syntheses of (THF)Â(H<sub>2</sub>L)Â(OU<sup>VI</sup>O)Â(An′)<sup>III</sup>Cp<sub>3</sub> (An′ = U and Np) were well reproduced by thermodynamic calculations
that yielded negative free energies in a tetrahydrofuran solution
but a positive one for their uranylplutonium analogue, which was synthetically
inaccessible. So, our thermodynamics would provide implications for
the synthetic possibility of other theoretically designed bimetallic
actinide complexes
Highly Diverse Bonding between Two U<sup>3+</sup> Ions When Ligated by a Flexible Polypyrrolic Macrocycle
A Schiff-base polypyrrolic ligand
(H<sub>4</sub>L) can accommodate
two U<sup>3+</sup> ions and form a Pacman-like complex [U<sub>2</sub>(L)]<sup>2+</sup> according to relativistic density functional theory.
Sixteen species, featuring four structural models in four electronic
states, are energetically stable. Ligand flexibility, lack of axial
restriction, and suitable U–N interactions allow the two U<sup>3+</sup> ions to stretch freely over a wide range, in contrast to
U<sub>2</sub>@C<sub><i>n</i></sub> (<i>n</i> =
60, 74, 80) studied previously. Diverse U<sup>3+</sup>–U<sup>3+</sup> interactions are found. The quintet state of the Out–In
model, which is calculated to be the global ground state both including
and excluding the spin–orbit coupling energy, likely shows
a weak single U<sub>2</sub> bond. In both <i>vertical</i> and <i>tilt</i> In–In species, a triple bond is
found. It is composed of two two-electron–two-center bonds
and two one-electron–two-center bonds; moreover, the <i>tilt</i> conformer is almost isoenergetic with Out–In.
The Out–Out species shows no U···U bonding.
Comparison with explicitly THF-solvated diuranium complexes is also
addressed
Structural Variations of the First Family of Heterometallic Uranyl Carboxyphosphinate Assemblies by Synergy between Carboxyphosphinate and Imidazole Ligands
Hydrothermal reactions of uranyl
acetate and a series of transition
metal acetates with a carboxyphosphinate and auxiliary N-donor ligands
gave rise to the formation of eight heterometallic uranyl-organic
assemblies, namely, CoÂ(im)<sub>2</sub>(UO<sub>2</sub>)<sub>3</sub>(L)<sub>4</sub> (<b>1</b>), ZnÂ(bpi)Â(UO<sub>2</sub>)Â(L)<sub>2</sub> (<b>2</b>), CdÂ(dib)Â(UO<sub>2</sub>)Â(L)<sub>2</sub> (<b>3</b>), MÂ(dib)Â(UO<sub>2</sub>)<sub>2</sub>(L)<sub>3</sub> (M =
Cd (<b>4</b>), Mn (<b>5</b>)), and [MÂ(dib)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>]Â[(UO<sub>2</sub>)<sub>3</sub>(L)<sub>4</sub>]·nH<sub>2</sub>O (M = Co (<b>6</b>, n = 2), Ni
(<b>7</b>, n = 2), Cu (<b>8</b>, n = 0)) [H<sub>2</sub>L = (2-carboxyethyl)Â(phenyl)Âphosphinic acid (CPP), im
= imidazole, bpi =1-(biphenyl-4-yl)-1H-imidazole, dib =1,4-diÂ(1H-imidazol-1-yl)Âbenzene].
Single-crystal X-ray diffraction (XRD) analysis of <b>1</b> reveals
a layered structure of UO<sub>6</sub>, UO<sub>7</sub>, and CoO<sub>4</sub>N<sub>2</sub> units that are linked by the carboxyphosphinate
ligands. Imidazole molecules modify the layer by coordinating to Co
centers. Similarly, <b>2</b> is a mixed zinc-uranyl carboxyphosphinate
with different topological two-dimensional structure and the decorated
moiety is a bpi coligand. When in the presence of bridging dib coligands,
the mixed cadmium–uranyl carboxyphosphinate sheets of <b>3</b> are pillared by dib forming a framework structure. The isostructures
of <b>4</b> and <b>5</b> are also pillared frameworks
constructed by a mixed heterometallic uranyl phosphinate layered subnet
that is different from that of <b>3</b>. The structures of <b>6</b>–<b>8</b> are isotype and very special in that
they consist of distinct [MÂ(dib)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>]<sub>n</sub><sup>2n+</sup> cationic and [(UO<sub>2</sub>)<sub>3</sub>(L)<sub>4</sub>]<sub>n</sub><sup>2n–</sup> anionic subnets.
Such two sheets are packed alternatively and interact via hydrogen
bond forming three-dimensional supramolecular structures
Self-Assembly of Hierarchically Structured Cellulose@ZnO Composite in Solid–Liquid Homogeneous Phase: Synthesis, DFT Calculations, and Enhanced Antibacterial Activities
To explore the interactions
of nanoparticles and bioresources and
elucidate their effects on the morphology of the resulting composite,
hierarchically structured cellulose@ZnO composites have been synthesized
by an environmentally friendly hydrothermal method in one step. First,
self-assembly induces the formation of hierarchical three-level structures,
including cellulose/ZnO nanofibers, layers, and microfibers. Then,
ZnO microparticles deposit onto the surface of the third-level cellulose/ZnO
microfibers and accomplish the fabrication of a cellulose@ZnO composite,
which eventually defines the hierarchical morphology of synthesized
materials. The self-assembly mechanism was comprehensively examined.
The electrostatic attraction between cellulose and ZnO, not hydrogen
bonding, was found to be the main driving force for the formation
of the first-level structure. A density functional theory study was
conducted to support the self-assembly mechanism by optimizing the
cellulose/ZnO structures at the molecular level, computing the corresponding
thermodynamic energies and examining the spectroscopic properties.
A hierarchically structured cellulose@ZnO composite is found to enhance
the antibacterial activities. The diameters of the inhibition zone
were found to be 48.8 and 45.5 mm against the Gram-positive bacterium <i>Staphylococcus aureus</i> (<i>S. aureus</i>) and the
Gram-negative bacterium <i>Escherichia coli</i> (<i>E. coli</i>), respectively. This study is expected to improve
food packaging materials while utilizing our newly synthesized cellulose@ZnO
composite
Theoretical Study of Structural, Spectroscopic and Reaction Properties of <i>trans</i>-<i>bis</i>(imido) Uranium(VI) Complexes
To
advance the understanding of the chemical behavior of actinides, a
series of <i>trans</i>-<i>bis</i>(imido) uraniumÂ(VI)
complexes, UÂ(NR)<sub>2</sub>(THF)<sub>2</sub>(<i>cis</i>-I<sub>2</sub>) (<b>2R</b>; R = H, Me, <sup><i>t</i></sup>Bu, Cy, and Ph), UÂ(NR)<sub>2</sub>(THF)<sub>3</sub>(<i>trans</i>-I<sub>2</sub>) (<b>3R</b>; R = H, Me, <sup><i>t</i></sup>Bu, Cy, and Ph) and UÂ(N<sup><i>t</i></sup>Bu)<sub>2</sub>(THF)<sub>3</sub>(<i>cis</i>-I<sub>2</sub>) (<b>3</b><sup><i><b>t</b></i></sup><b>Bu′</b>), were investigated using relativistic density
functional theory. The axial Uî—»N bonds in these complexes have
partial triple bonding character. The calculated bond lengths, bond
orders, and stretching vibrational frequencies reveal that the Uî—»N
bonds of the <i>bis</i>-imido complexes can be tuned by
the variation of their axial substituents. This has been evidenced
by the analysis of electronic structures. <b>2H</b>, for instance,
was calculated to show iodine-based high-lying occupied orbitals and
UÂ(<i>f</i>)-type low-lying unoccupied orbitals. Its Uî—»N
bonding orbitals, formed by UÂ(<i>f</i>) and NÂ(<i>p</i>), occur in a region of the relatively low energy. Upon varying the <i><b>axial</b></i> substituent from H to <sup><i>t</i></sup>Bu and Ph, the Uî—»N bonding orbitals of <b>2</b><sup><i><b>t</b></i></sup><b>Bu</b> and <b>2Ph</b> are greatly destabilized. We further compared the Uî—»E
(E = N and O) bonds of <b>2H</b> with <b>3H</b> and their
uranyl analogues, to address effects of the <i><b>equatorial</b></i> tetrahydrofuran (THF) ligand and the E group. It is found
that the Uî—»N bonds are slightly weaker than the Uî—»O
bonds of their uranyl analogues. This is in line with the finding
that <i>cis</i>-UNR<sub>2</sub> isomers, although energetically
unfavorable, are more accessible than <i>cis</i>-UO<sub>2</sub> would be. It is also evident that <b>2H</b> and <b>3H</b> display lower Uî—»(NH) stretching vibrations at 740
cm<sup>–1</sup> than the UO at 820 cm<sup>–1</sup> of uranyl complexes. With the inclusion of both solvation and spin–orbit
coupling, the free energies of the formation reactions of the <i>bis</i>-imido uranium complexes were calculated. The formation
of the experimentally synthesized <b>3Me</b>, <b>3Ph</b>, and <b>2</b><sup><i><b>t</b></i></sup><b>Bu</b> are found to be thermodynamically favorable. Finally, the
absorption bands previously obtained from experimental studies were
well reproduced by time-dependent density functional theory calculations