13 research outputs found
Hydrogen-Bonded Structures of Water Molecules in Hydroxy-Functionalized Nanochannels of Columnar Liquid Crystalline Nanostructured Membranes Studied by Soft X‑ray Emission Spectroscopy
Here, we report a
synchrotron-based high-resolution soft X-ray
emission spectroscopy study on hydrogen-bonded structures of water
molecules in the self-organized, hydroxy-group-functionalized one-dimensional
nanochannels of liquid crystalline nanostructured membranes. The water
molecules confined in the uncharged hydroxy-functionalized nanochannels
(which have a diameter of about 1.5 nm) exhibit hydrogen-bonded structures
close to those of bulk liquid water, even directly interacting with
diol groups. These hydrogen-bonded structures contrast with the more
distorted hydrogen bonding of water molecules confined in self-organized
channels with a diameter of 0.6 nm formed by an analogous nanostructured
membrane with a cationic moiety, which was explained by the ability
of the channel functional groups to donate and accept hydrogen bonds
in a confined space and the nanochannel diameter
First-Principles Investigation of Strong Excitonic Effects in Oxygen 1s X‑ray Absorption Spectra
We
calculated the oxygen 1s X-ray absorption spectra (XAS) of acetone
and acetic acid molecules in vacuum by utilizing the first-principles <i>GW</i>+Bethe–Salpeter method with an all-electron mixed
basis. The calculated excitation energies show good agreement with
the available experimental data without an artificial shift. The remaining
error, which is less than 1% or 2–5 eV, is a significant improvement
from those of time-dependent (TD) density functional methods (5% error
or 27–29 eV for TD-LDA and 2.4–2.8% error or 13–15
eV for TD-B3LYP). Our method reproduces the first and second isolated
peaks and broad peaks at higher photon energies, corresponding to
Rydberg excitations. We observed a failure of the one-particle picture
(or independent particle approximation) from our assignment of the
five lowest exciton peaks and significant excitonic or state-hybridization
effects inherent in the core electron excitations
Enhancement of the Hydrogen-Bonding Network of Water Confined in a Polyelectrolyte Brush
Water existing in
the vicinity of polyelectrolytes exhibits unique
structural properties, which demonstrate key roles in chemistry, biology,
and geoscience. In this study, X-ray absorption and emission spectroscopy
was employed to observe the local hydrogen-bonding structure of water
confined in a charged polyelectrolyte brush. Even at room temperature,
a majority of the water molecules confined in the polyelectrolyte
brush exhibited one type of hydrogen-bonding configuration: a slightly
distorted, albeit ordered, configuration. The findings from this study
provide new insight in terms of the correlation between the function
and local structure of water at the interface of biological materials
under physiological conditions
Direct Observation of Cr<sup>3+</sup> 3d States in Ruby: Toward Experimental Mechanistic Evidence of Metal Chemistry
The
role of transition metals in chemical reactions is often derived
from probing the metal 3d states. However, the relation between metal
site geometry and 3d electronic states, arising from multielectronic
effects, makes the spectral data interpretation and modeling of these
optical excited states a challenge. Here we show, using the well-known
case of red ruby, that unique insights into the density of transition
metal 3d excited states can be gained with 2p3d resonant inelastic
X-ray scattering (RIXS). We compare the experimental determination
of the 3d excited states of Cr<sup>3+</sup> impurities in Al<sub>2</sub>O<sub>3</sub> with 190 meV resolution 2p3d RIXS to optical absorption
spectroscopy and to simulations. Using the crystal field multiplet
theory, we calculate jointly for the first time the Cr<sup>3+</sup> multielectronic states, RIXS, and optical spectra based on a unique
set of parameters. We demonstrate that (i) anisotropic 3d multielectronic
interactions causes different scaling of Slater integrals, and (ii)
a previously not observed doublet excited state exists around 3.35
eV. These results allow to discuss the influence of interferences
in the RIXS intermediate state, of core–hole lifetime broadenings,
and of selection rules on the RIXS intensities. Finally, our results
demonstrate that using an intermediate excitation energy between L<sub>3</sub> and L<sub>2</sub> edges allows measurement of the density
of 3d excited states as a fingerprint of the metal local structure.
This opens up a new direction to pump-before-destroy investigations
of transition metal complex structures and reaction mechanisms
Direct Observation of Cr<sup>3+</sup> 3d States in Ruby: Toward Experimental Mechanistic Evidence of Metal Chemistry
The
role of transition metals in chemical reactions is often derived
from probing the metal 3d states. However, the relation between metal
site geometry and 3d electronic states, arising from multielectronic
effects, makes the spectral data interpretation and modeling of these
optical excited states a challenge. Here we show, using the well-known
case of red ruby, that unique insights into the density of transition
metal 3d excited states can be gained with 2p3d resonant inelastic
X-ray scattering (RIXS). We compare the experimental determination
of the 3d excited states of Cr<sup>3+</sup> impurities in Al<sub>2</sub>O<sub>3</sub> with 190 meV resolution 2p3d RIXS to optical absorption
spectroscopy and to simulations. Using the crystal field multiplet
theory, we calculate jointly for the first time the Cr<sup>3+</sup> multielectronic states, RIXS, and optical spectra based on a unique
set of parameters. We demonstrate that (i) anisotropic 3d multielectronic
interactions causes different scaling of Slater integrals, and (ii)
a previously not observed doublet excited state exists around 3.35
eV. These results allow to discuss the influence of interferences
in the RIXS intermediate state, of core–hole lifetime broadenings,
and of selection rules on the RIXS intensities. Finally, our results
demonstrate that using an intermediate excitation energy between L<sub>3</sub> and L<sub>2</sub> edges allows measurement of the density
of 3d excited states as a fingerprint of the metal local structure.
This opens up a new direction to pump-before-destroy investigations
of transition metal complex structures and reaction mechanisms
Enhancement in Kinetics of the Oxygen Reduction Reaction on a Nitrogen-Doped Carbon Catalyst by Introduction of Iron via Electrochemical Methods
The iron (Fe) electrodeposition–electrochemical
dissolution
has been employed on nitrogen-doped carbon material (P-PI) prepared
via multi-step pyrolysis of a polyimide precursor to achieve the introduction
of Fe species, and its influence on the oxygen reduction reaction
(ORR) is investigated by cyclic and rotating ring-disk electrode voltammetry
in 0.5 M H<sub>2</sub>SO<sub>4</sub>. After the electrochemical treatment,
the overpotential and H<sub>2</sub>O<sub>2</sub> production percentage
of ORR on the P-PI are decreased and the number of electrons transferred
is increased in the meanwhile. In combination with the results of
X-ray absorption fine structure spectra, the presence of Fe–N<sub><i>x</i></sub> sites (Fe ions coordinated by nitrogen)
is believed to be responsible for the improved ORR performance. Further
kinetic analysis indicates that a two-electron reduction of O<sub>2</sub> is predominant on the untreated P-PI with coexistence of
a direct four-electron transformation of O<sub>2</sub> to H<sub>2</sub>O, while the introduction of Fe species leads to a larger increase
in the rate constant for the four-electron reduction than that for
the two-electron process, being in good agreement with the view that
Fe–N<sub><i>x</i></sub> sites are active for four-electron
ORR
Distinguishing between High- and Low-Spin States for Divalent Mn in Mn-Based Prussian Blue Analogue by High-Resolution Soft X‑ray Emission Spectroscopy
We
combine Mn <i>L</i><sub>2,3</sub>-edge X-ray absorption,
high resolution Mn 2p–3d–2p resonant X-ray emission,
and configuration–interaction full-multiplet (CIFM) calculation
to analyze the electronic structure of Mn-based Prussian blue analogue.
We clarified the Mn 3d energy diagram for the Mn<sup>2+</sup> low-spin
state separately from that of the Mn<sup>2+</sup> high-spin state
by tuning the excitation energy for the X-ray emission measurement.
The obtained X-ray emission spectra are generally reproduced by the
CIFM calculation for the Mn<sup>2+</sup> low spin state having a stronger
ligand-to-metal charge-transfer effect between Mn <i>t</i><sub>2g</sub> and CN π orbitals than the Mn<sup>2+</sup> high
spin state. The d–d-excitation peak nearest to the elastic
scattering was ascribed to the Mn<sup>2+</sup> LS state by the CIFM
calculation, indicating that the Mn<sup>2+</sup> LS state with a hole
on the <i>t</i><sub>2g</sub> orbital locates near the Fermi
level
In Situ Hard X‑ray Photoelectron Study of O<sub>2</sub> and H<sub>2</sub>O Adsorption on Pt Nanoparticles
To improve the efficiency of Pt-based
cathode catalysts in polymer
electrolyte fuel cells, understanding of the oxygen reduction process
at surfaces and interfaces in the molecular level is essential. In
this study, H<sub>2</sub>O and O<sub>2</sub> adsorption and dissociation
as the first step of the reduction process were investigated by in
situ hard X-ray photoelectron spectroscopy (HAXPES). Pt 5d valence
band and Pt 3d, Pt 4f core HAXPES spectra of Pt nanoparticles upon
H<sub>2</sub>O and O<sub>2</sub> adsorption revealed that H<sub>2</sub>O adsorption has a negligible effect on the electronic structure
of Pt, while O<sub>2</sub> adsorption has a significant effect, reflecting
the weak and strong chemisorption of H<sub>2</sub>O and O<sub>2</sub> on the Pt nanoparticle, respectively. Combined with ab initio theoretical
calculations, it is concluded that Pt 5d states responsible for Pt–O<sub>2</sub> bonding reside within 2 eV from the Fermi level
Measurement of the Ligand Field Spectra of Ferrous and Ferric Iron Chlorides Using 2p3d RIXS
Ligand field spectra provide direct
information about the electronic structure of transition metal complexes.
However, these spectra are difficult to measure by conventional optical
techniques due to small cross sections for d-to-d transitions and
instrumental limitations below 4000 cm<sup>–1</sup>. 2p3d resonant
inelastic X-ray scattering (RIXS) is a second order process that utilizes
dipole allowed 2p to 3d transitions to access d–d excited states.
The measurement of ligand field excitation spectra by RIXS is demonstrated
for a series of tetrahedral and octahedral FeÂ(II) and FeÂ(III) chlorides,
which are denoted FeÂ(III)-<i>T</i><sub><i>d</i></sub>, FeÂ(II)-<i>T</i><sub><i>d</i></sub>, FeÂ(III)-<i>O</i><sub><i>h</i></sub>, and FeÂ(II)-<i>O</i><sub><i>h</i></sub>. The strong 2p spin–orbit coupling
allows the measurement of spin forbidden transitions in RIXS spectroscopy.
The FeÂ(III) spectra are dominated by transitions from the sextet ground
state to quartet excited states, and the FeÂ(II) spectra contain transitions
to triplet states in addition to the spin allowed <sup>5</sup>Γ
→ <sup>5</sup>Γ transition. Each experimental spectrum
is simulated using a ligand field multiplet model to extract the ligand
field splitting parameter 10Dq and the Racah parameters <i>B</i> and <i>C</i>. The 10Dq values for FeÂ(III)-<i>T</i><sub><i>d</i></sub>, FeÂ(II)-<i>T</i><sub><i>d</i></sub>, and FeÂ(III)-<i>O</i><sub><i>h</i></sub> are found to be −0.7, −0.32, and 1.47 eV, respectively.
In the case of FeÂ(II)-<i>O</i><sub><i>h</i></sub>, a single 10Dq parameter cannot be assigned because FeÂ(II)-<i>O</i><sub><i>h</i></sub> is a coordination polymer
exhibiting axially compressed FeÂ(II)Cl <sub>6</sub> units. The <sup>5</sup>T → <sup>5</sup>E transition is split by the axial
compression resulting in features at 0.51 and 0.88 eV. The present
study forms the foundation for future applications of 2p3d RIXS to
molecular iron sites in more complex systems, including iron-based
catalysts and enzymes
Probing the Valence Electronic Structure of Low-Spin Ferrous and Ferric Complexes Using 2p3d Resonant Inelastic X‑ray Scattering (RIXS)
Understanding the detailed electronic
structure of transition metal
ions is essential in numerous areas of inorganic chemistry. In particular,
the ability to map out the many particle d–d spectrum of a
transition metal catalyst is key to understanding and predicting reactivity.
However, from a practical perspective, there are often experimental
limitations on the ability to determine the energetic ordering, and
multiplicity of all the excited states. These limitations derive in
part from parity and spin-selection rules, as well as from the limited
energy range of many standard laboratory instruments. Herein, we demonstrate
the ability of 2p3d resonant inelastic X-ray scattering (RIXS) to
obtain detailed insights into the many particle spectrum of simple
inorganic molecular iron complexes. The present study focuses on low-spin
ferrous and ferric iron complexes, including [Fe<sup>III/II</sup>Â(tacn)<sub>2</sub>]<sup>3+/2+</sup> and [Fe<sup>III/II</sup>Â(CN)<sub>6</sub>]<sup>3–/4–</sup>. This series thus allows us to assess
the contribution of d-count and ligand donor type, by comparing the
purely σ-donating tacn ligand to the π-accepting cyanide.
In order to highlight the conceptual difference between RIXS and traditional
optical spectroscopy, we compare first RIXS results with UV–vis
and magnetic circular dichroism spectroscopy. We then highlight the
ability of 2p3d RIXS to (1) separate d–d transitions from charge
transfer transitions and (2) to determine the many particle d–d
spectrum over a much wider energy range than is possible by optical
spectroscopy. Our experimental results are correlated with semiempirical
multiplet simulations and <i>ab initio</i> complete active
space self-consistent field calculations in order to obtain detailed
assignments of the excited states. These results show that Δ<i>S</i> = 1, and possibly Δ<i>S</i> = 2, transitions
may be observed in 2p3d RIXS spectra. Hence, this methodology has
great promise for future applications in all areas of transition metal
inorganic chemistry