7 research outputs found
Structural Evolution of Homoleptic Heterodinuclear Copper–Nickel Carbonyl Anions Revealed Using Photoelectron Velocity-Map Imaging
The
homoleptic heterodinuclear copper–nickel carbonyl anions CuNiÂ(CO)<sub><i>n</i></sub><sup>–</sup> (<i>n</i> =
2–4) were generated in a pulsed-laser vaporization source and
investigated using photoelectron velocity-map imaging spectroscopy.
The electron affinities of CuNiÂ(CO)<sub>2</sub> (2.15 ± 0.03
eV), CuNiÂ(CO)<sub>3</sub> (2.30 ± 0.03 eV), and CuNiÂ(CO)<sub>4</sub> (1.90 ± 0.04 eV) were deduced from the photoelectron
spectra. Theoretical calculations at the B3LYP level were carried
out to elucidate the structures and the electronic properties of CuNiÂ(CO)<sub><i>n</i></sub><sup>0/1–</sup> (<i>n</i> = 1–4) and to support the experimental observations. Comprehensive
comparisons between experiments and calculations suggest that there
is a turnover point of the absorption site during the progressive
carbonylation process. The carbonyl groups are determined to be preferentially
bonded to the nickel atom. When the nickel center satisfies the 18-electron
configuration, the copper atom starts to adsorb additional CO molecules.
These results will shed light on the bonding mechanisms of the heterometallic
carbonyl clusters
Photoelectron Velocity Map Imaging Spectroscopy of Lead Tetracarbonyl–Iron Anion PbFe(CO)<sub>4</sub><sup>–</sup>
Joint
research of photoelectron velocity map imaging spectroscopy and density
functional theory has been performed to probe the geometrical structures
and electronic properties for heterodinuclear iron–lead carbonyl
cluster PbFeÂ(CO)<sub>4</sub><sup>–</sup>, which serves as a
monomer of the metal–metal bonded oligomer. The photoelectron
detachment of PbFeÂ(CO)<sub>4</sub><sup>–</sup> is recorded
at two different photon energies with rich spectral features. The
ground-state transition obtained at 532 nm reveals a broad vibrationally
resolved spectral band, which corresponds to the lead–iron
stretching, while the 355 nm spectrum displays many more transitions
on the higher-energy side, which correspond to the electronic excited
states of PbFeÂ(CO)<sub>4</sub>. Theoretical calculations at the B3LYP
level are performed to explore the ground states of both the anionic
and neutral PbFeÂ(CO)<sub>4</sub> and to support spectral identification
of the fine resolved photoelectron spectra. Moreover, the unique chemical
bonding between lead and iron in PbFeÂ(CO)<sub>4</sub> is discussed
with the aid of natural bond orbital analyses
Structural and Chemical Bonding Properties of AuS<sub>2</sub>H<sup>0/–</sup>: A Photoelectron Velocity-Map Imaging Spectroscopic and Theoretical Study
Mass-selected photoelectron velocity-map imaging spectroscopy
was
employed to investigate the geometrical and electronic properties
of AuS2H–/0. The comprehensive comparison
between the experiment and theoretical calculations establishes that
the ground-state AuS2H– anion has a mixed-ligand
structure [SAuSH]− with an unsymmetrical S–Au–S
unit. Further chemical bonding analyses on AuS2H and comparison
with the isoelectronic AuS2– suggest
that the unique S–Au–S unit in these species features
two three-center, three-electron π-bonding, and one three-center,
two-electron σ-bonding. The isoelectronic replacement of the
extra electron in AuS2– by the H atom
can lead to σ bonding evolution from the electron-sharing bond
to the dative bond. These findings are conducive to the fundamental
understanding of the intrinsic stability of thiolate-protected gold
nanoclusters and their delicate ligand design to achieve desirable
properties
Observing the Transition from Equatorial to Axial CO Chemisorption: Infrared Photodissociation Spectroscopy of Yttrium Oxide–Carbonyls
A series
of yttrium oxide–carbonyls are prepared via a laser
vaporization supersonic cluster source in the gas phase and identified
by mass-selected infrared photodissociation (IRPD) spectroscopy in
the C–O stretching region and by comparing the observed IR
spectra with those from quantum chemical calculations. For YOÂ(CO)<sub>4</sub><sup>+</sup>, all four CO ligands prefer to occupy the equatorial
site of the YO<sup>+</sup> unit, leading to a quadrangular pyramid
with <i>C</i><sub>4<i>v</i></sub> symmetry. Two
energetically nearly degenerate isomers are responsible for YOÂ(CO)<sub>5</sub><sup>+</sup>, in which the fifth CO ligand is either inserted
into the equatorial plane of YOÂ(CO)<sub>4</sub><sup>+</sup> or coordinated
opposite the oxygen on the <i>C</i><sub>4</sub> axis. YOÂ(CO)<sub>6</sub><sup>+</sup> has a pentagonal bipyramidal structure with <i>C</i><sub>5<i>v</i></sub> symmetry, which includes
five equatorial CO ligands and one axial CO ligand. The present IRPD
spectroscopic and theoretical study of YOÂ(CO)<sub><i>n</i></sub><sup>+</sup> extends the first shell coordination number of
CO ligands in metal monoxide carbonyls to six. The transition from
equatorial to axial CO chemisorption in these yttrium oxide–carbonyls
is fortunately observed at <i>n</i> = 5, providing new insight
into ligand interactions and coordination for the transition metal
oxides
FeNC catalysts decorated with NiFe<sub>2</sub>O<sub>4</sub> to enhance bifunctional activity for Zn–Air batteries
Rechargeable Zn–air battery is a promising next-generation energy storage device attributed to its high energy density, excellent safety, and low cost. However, its commercialization is hampered by sluggish kinetics of the oxygen reduction reaction (ORR) and oxygen evolution reaction (OER) at air electrodes. Herein, we have designed, fabricated, and demonstrated a highly efficient ORR/OER electrocatalyst, NiFe2O4/FeNC, using low-cost materials via a facile synthesis route. NiFe2O4 is successfully loaded on Fe/N-doped carbon (FeNC) through bonding to Fe3C in FeNC. Due to the existence of high ORR active sites such as FeN4 and Fe and N-doped carbon moieties, the half-wave potential of the ORR reaches a high value of 0.83 V. While benefited from NiFe2O4 with high OER activity and the synergistic effect between NiFe2O4 and FeNC, the overpotential is 310 mV at 10 mA cm–2 in the OER. The voltage difference between charging–discharging operations in the Zn–air battery employing the NiFe2O4/FeNC electrocatalyst only increases by 0.16 V after cycling for 100 h (600 cycles) at 10 mA cm–2, which is much lower than 1.28 V using the best commercial Pt/C and RuO2 catalysts. </p
Vibrationally Resolved Photoelectron Imaging of Cu<sub>2</sub>H<sup>–</sup> and AgCuH<sup>–</sup> and Theoretical Calculations
Vibrationally resolved photoelectron
spectra have been obtained
for Cu<sub>2</sub>H<sup>–</sup> and AgCuH<sup>–</sup> using photoelectron imaging at 355 nm. Two transition bands X and
A are observed for each spectrum. The X bands in both spectra show
the vibration progressions of the Cu–H stretching mode and
the broad peaks of these progressions indicate significant structural
changes from Cu<sub>2</sub>H<sup>–</sup> and AgCuH<sup>–</sup> to their neutral ground states. The A bands in the spectra of Cu<sub>2</sub>H<sup>–</sup> and CuAgH<sup>–</sup> show stretching
progressions of Cu–Cu and Ag–Cu, respectively. The contours
of these two progressions are pretty narrow, indicating relatively
small structural changes from Cu<sub>2</sub>H<sup>–</sup> and
AgCuH<sup>–</sup> to their neutral excited states. Calculations
based on density functional theory indicate that the ground states
of Cu<sub>2</sub>H<sup>–</sup> and AgCuH<sup>–</sup> and the first excited states of their neutrals are linear, whereas
their neutral ground states are bent. The photoelectron detachment
energies and vibrational frequencies from these calculations are in
good agreement with the experimental observations. Especially, the
theoretical predication of linear structures for the anions and the
neutral excited states are supported by the spectral features of A
bands, in which the bending modes are inactive. Comparisons among
the vertical detachment energies of Cu<sub>2</sub>H<sup>–</sup>, AgCuH<sup>–</sup>, and their analogs help to elucidate electronic
characteristics of coinage metal elements and hydrogen in small clusters
Supplementary information files for FeNC catalysts decorated with NiFe2O4 to enhance bifunctional activity for Zn–Air batteries
Supplementary files for article FeNC catalysts decorated with NiFe2O4 to enhance bifunctional activity for Zn–Air batteriesÂ
Rechargeable Zn–air battery is a promising next-generation energy storage device attributed to its high energy density, excellent safety, and low cost. However, its commercialization is hampered by sluggish kinetics of the oxygen reduction reaction (ORR) and oxygen evolution reaction (OER) at air electrodes. Herein, we have designed, fabricated, and demonstrated a highly efficient ORR/OER electrocatalyst, NiFe2O4/FeNC, using low-cost materials via a facile synthesis route. NiFe2O4 is successfully loaded on Fe/N-doped carbon (FeNC) through bonding to Fe3C in FeNC. Due to the existence of high ORR active sites such as FeN4 and Fe and N-doped carbon moieties, the half-wave potential of the ORR reaches a high value of 0.83 V. While benefited from NiFe2O4 with high OER activity and the synergistic effect between NiFe2O4 and FeNC, the overpotential is 310 mV at 10 mA cm–2 in the OER. The voltage difference between charging–discharging operations in the Zn–air battery employing the NiFe2O4/FeNC electrocatalyst only increases by 0.16 V after cycling for 100 h (600 cycles) at 10 mA cm–2, which is much lower than 1.28 V using the best commercial Pt/C and RuO2 catalysts.  </p