7 research outputs found
Boosting Graphene Reactivity with Oxygen by Boron Doping: Density Functional Theory Modeling of the Reaction Path.
Graphene
(G) reactivity toward oxygen is very poor, which limits
its use as electrode for the oxygen reduction reaction (ORR). Contrarily,
boron-doped graphene was found to be an excellent catalyst for the
ORR. Through a density functional study, comparing molecular and periodic
approaches and different functionals (B3LYP vs PBE), we show how substitutional
boron in the carbon sheet can boost the reactivity with oxygen leading
to the formation of bulk borates covalently bound to graphene (BO<sub>3</sub>–G) in oxygen-rich conditions. These species are highly
interesting intermediates for the OO breaking step in the
reduction process of O<sub>2</sub> to form H<sub>2</sub>O as they
are energetically stable
Treatment of Layered Structures Using a Semilocal meta-GGA Density Functional
Density functional theory calculations on solids consisting of covalently bonded layers held together by dispersive interactions are presented. Utilizing the kinetic energy density in addition to the density and its gradients gives the meta-generalized gradient approximation (MGGA) M06-L enough flexibility to treat correctly both the covalent and the dispersive interactions in layered solids, thus making it a significant step forward compared to the local density and generalized gradient approximations. We show how the MGGA can take advantage of the extra information in the kinetic energy density to discriminate between dispersive and covalent interactions and thereby prove that the performance of M06-L for dispersive interactions, as opposed to that for the local density approximation, is not based on an accidental cancellation of errors
Catalysis under Cover: Enhanced Reactivity at the Interface between (Doped) Graphene and Anatase TiO<sub>2</sub>
The “catalysis
under cover” involves chemical processes
which take place in the confined zone between a 2D material, such
as graphene, h-BN, or MoS<sub>2</sub>, and the surface of an underlying
support, such as a metal or a semiconducting oxide. The hybrid interface
between graphene and anatase TiO<sub>2</sub> is extremely important
for photocatalytic and catalytic applications because of the excellent
and complementary properties of the two materials. We investigate
and discuss the reactivity of O<sub>2</sub> and H<sub>2</sub>O on
top and at the interface of this hybrid system by means of a wide
set of dispersion-corrected hybrid density functional calculations.
Both pure and boron- or nitrogen-doped graphene are interfaced with
the most stable (101) anatase surface of TiO<sub>2</sub> in order
to improve the chemical activity of the C-layer. Especially in the
case of boron, an enhanced reactivity toward O<sub>2</sub> dissociation
is observed as a result of both the contribution of the dopant and
of the confinement effect in the bidimensional area between the two
surfaces. Extremely stable dissociation products are observed where
the boron atom bridges the two systems by forming very stable BO
covalent bonds. Interestingly, the B defect in graphene could also
act as the transfer channel of oxygen atoms from the top side across
the C atomic layer into the G/TiO<sub>2</sub> interface. On the contrary,
the same conditions are not found to favor water dissociation, proving
that the “catalysis under cover” is not a general effect,
but rather highly depends on the interfacing material properties,
on the presence of defects and impurities and on the specific reaction
involved
Water at the Interface Between Defective Graphene and Cu or Pt (111) Surfaces
The
presence of defects in the graphenic layers deposited on metal surfaces
modifies the nature of the interaction. Unsaturated carbon atoms,
due to vacancies in the lattice, form strong organometallic bonds
with surface metal atoms that highly enhance the binding energy between
the two materials. We investigate by means of a wide set of dispersion-corrected
density functional theory calculations how such strong chemical bonds
affect both the electronic properties of these hybrid interfaces and
the chemical reactivity with water, which is commonly present in the
working conditions. We compare different metal substrates (Cu vs Pt)
that present a different type of interaction with graphene and with
defective graphene. This comparative analysis allows us to unravel
the controlling factors of water reactivity, the role played by the
carbon vacancies and by the confinement or “graphene cover
effect”. Water is capable of breaking the C–Cu bond
by dissociating at the undercoordinated carbon atom of the vacancy,
restoring the weak van der Waals type of interaction between the two
materials that allows for an easy detachment of graphene from the
metal, but the same is not true in the case of Pt, where C–Pt
bonds are much stronger. These conclusions can be used to rationalize
water reactivity at other defective graphene/metal interfaces
π Magnetism of Carbon Monovacancy in Graphene by Hybrid Density Functional Calculations
Understanding
magnetism in defective graphene is paramount to improve
and broaden its technological applications. A single vacancy in graphene
is expected to lead to a magnetic moment with both a σ (1 μ<sub>B</sub>) and a π (1 μ<sub>B</sub>) component. Theoretical
calculations based on standard LDA or GGA functional on periodic systems
report a partial quenching of the π magnetization (0.5 μ<sub>B</sub>) due to the crossing of two spin split bands at the Fermi
level. In contrast, STS experiments (Phys. Rev. Lett. 2016, 117, 166801) have recently proved the existence
of two defect spin states that are separated in energy by 20–60
meV. In this work, we show that self-interaction corrected hybrid
functional methods (B3LYP-D*) are capable of correctly reproducing
this finite energy gap and, consequently, provide a π magnetization
of 1 μ<sub>B</sub>. The crucial role played by the exact exchange
is highlighted by comparison with PBE-D2 results and by the magnetic
moment dependence with the exact exchange portion in the functional
used. The ground state ferromagnetic planar solution is compared to
the antiferromagnetic and to the diamagnetic ones, which present an
out-of-plane distortion. Periodic models are then compared to graphene
nanoflakes of increasing size (up to C<sub>383</sub>H<sub>48</sub>). For large models, the triplet spin configuration (total magnetization
2 μ<sub>B</sub>) is the most stable, independently of the functional
used, which further corroborates the conclusions of this work and
puts an end to the long-debated issue of the magnetic properties of
an isolated C monovacancy in graphene
Single and Multiple Doping in Graphene Quantum Dots: Unraveling the Origin of Selectivity in the Oxygen Reduction Reaction
Singly and multiply doped graphene
oxide quantum dots have been
synthesized by a simple electrochemical method using water as solvent.
The obtained materials have been characterized by photoemission spectroscopy
and scanning tunneling microscopy, in order to get a detailed picture
of their chemical and structural properties. The electrochemical activity
toward the oxygen reduction reaction of the doped graphene oxide quantum
dots has been investigated by cyclic voltammetry and rotating disk
electrode measurements, showing a clear decrease of the overpotential
as a function of the dopant according to the sequence: N ∼
B > B,N. Moreover, assisted by density functional calculations
of
the Gibbs free energy associated with every electron transfer, we
demonstrate that the selectivity of the reaction is controlled by
the oxidation states of the dopants: as-prepared graphene oxide quantum
dots follow a two-electron reduction path that leads to the formation
of hydrogen peroxide, whereas after the reduction with NaBH<sub>4,</sub> the same materials favor a four-electron reduction of oxygen to
water
Stereodirection of an α‑Ketoester at Sub-molecular Sites on Chirally Modified Pt(111): Heterogeneous Asymmetric Catalysis
Chirally
modified Pt catalysts are used in the heterogeneous asymmetric
hydrogenation of α-ketoesters. Stereoinduction is believed to
occur through the formation of chemisorbed modifier–substrate
complexes. In this study, the formation of diastereomeric complexes
by coadsorbed methyl 3,3,3-trifluoropyruvate, MTFP, and (<i>R</i>)-(+)-1-(1-naphthyl)ethylamine, (<i>R</i>)-NEA, on Pt(111)
was studied using scanning tunneling microscopy and density functional
theory methods. Individual complexes were imaged with sub-molecular
resolution at 260 K and at room temperature. The calculations find
that the most stable complex isolated in room-temperature experiments
is formed by the minority rotamer of (<i>R</i>)-NEA and
pro-S MTFP. The stereodirecting forces in this complex are identified
as a combination of site-specific chemisorption of MTFP and multiple
non-covalent attractive interactions between the carbonyl groups of
MTFP and the amine and aromatic groups of (<i>R</i>)-NEA