7 research outputs found
Reactions of Vanadium Dioxide Molecules with Acetylene: Infrared Spectra of VO<sub>2</sub>(η<sup>2</sup>‑C<sub>2</sub>H<sub>2</sub>)<sub><i>x</i></sub> (<i>x</i> = 1, 2) and OV(OH)CCH in Solid Neon
Reactions
of vanadium dioxide molecules with acetylene have been
studied by matrix isolation infrared spectroscopy. Reaction intermediates
and products are identified on the basis of isotopic substitutions
as well as density functional frequency calculations. Ground state
vanadium dioxide molecule reacts with acetylene in forming the side-on-bonded
VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) and
VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complexes spontaneously on annealing in solid neon. The VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) complex is
characterized to have a <sup>2</sup>B<sub>2</sub> ground state with <i>C</i><sub>2<i>v</i></sub> symmetry, whereas the VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complex has a <sup>2</sup>A ground state with <i>C</i><sub>2</sub> symmetry. The VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) and VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complexes are photosensitive. The
VO<sub>2</sub>(η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) complex
rearranges to the OVÂ(OH)ÂCCH molecule upon UV–vis light excitation
Infrared Spectra and Structures of the Neutral and Charged CrCO<sub>2</sub> and Cr(CO<sub>2</sub>)<sub>2</sub> Isomers in Solid Neon
The
reactions from codeposition of laser-ablated chromium atoms
with carbon dioxide in excess neon are studied by infrared absorption
spectroscopy. The species formed are identified by the effects of
isotopic substitution on their infrared spectra. Density functional
calculations are performed to support the spectral assignments and
to interpret the geometric and electronic structures of the experimentally
observed species. Besides the previously reported insertion products
OCrCO and O<sub>2</sub>CrÂ(CO)<sub>2</sub>, the one-to-one CrÂ(CO<sub>2</sub>) complex and the one-to-two CrÂ(CO<sub>2</sub>)<sub>2</sub> complex as well as the CrOCrCO and OCCrCO<sub>3</sub> complexes
are also formed. The CrÂ(CO<sub>2</sub>) complex is characterized to
be side-on η<sup>2</sup>-C,O-coordinated. The CrÂ(CO<sub>2</sub>)<sub>2</sub> complex is identified to involve a side-on η<sup>2</sup>-C,O-coordinated CO<sub>2</sub> and an end-on η<sup>1</sup>-O-coordinated CO<sub>2</sub>. OCCrCO<sub>3</sub> is a carbonate
carbonyl complex predicted to have a planar structure with a η<sup>2</sup>-O,O-coordinated carbonate ligand. The CrOCrCO complex is
predicted to be linear with a high-spin ground state. Besides the
neutral molecules, charged species are also produced. The CrÂ(CO<sub>2</sub>)<sup>+</sup> and CrÂ(CO<sub>2</sub>)<sub>2</sub><sup>+</sup> cation complexes are characterized to have linear end-on η<sup>1</sup>-O-coordinated structures with blue-shifted antisymmetric
CO<sub>2</sub> stretching vibrational frequencies. The OCrCO<sup>–</sup> anion is bent with the Cr–O and CO stretching frequencies
red-shifted from those of OCrCO neutral molecule
Formation and Infrared Spectroscopic Characterization of Three Oxygen-Rich BiO<sub>4</sub> Isomers in Solid Argon
The
reactions of bismuth atoms and O<sub>2</sub> have been investigated
using matrix isolation infrared spectroscopy and density functional
theory calculations. The ground state bismuth atoms react with dioxygen
to form the BiOO and BiÂ(O<sub>2</sub>)<sub>2</sub> complexes spontaneously
on annealing. The BiOO molecule is characterized to be an end-on bonded
superoxide complex, while the BiÂ(O<sub>2</sub>)<sub>2</sub> molecule
is characterized to be a superoxo bismuth peroxide complex, [Bi<sup>3+</sup>(O<sub>2</sub><sup>–</sup>)Â(O<sub>2</sub><sup>2‑</sup>)]. Under UV–visible light irradiation, the BiÂ(O<sub>2</sub>)<sub>2</sub> complex rearranges to the more stable OBiOOO isomer,
an end-on bonded bismuth monoxide-ozonide complex. The end-on-bonded
OBiOOO complex further rearranges to a more stable side-on bonded
OBiO<sub>3</sub> isomer upon sample annealing. In addition, the bent
bismuth dioxide anion is also formed and assigned
Carbon Dioxide Activation by Scandium Atoms and Scandium Monoxide Molecules: Formation and Spectroscopic Characterization of ScCO<sub>3</sub> and OCScCO<sub>3</sub> in Solid Neon
The
reactions of carbon dioxide with scandium monoxide molecules
and scandium atoms are investigated using matrix isolation infrared
spectroscopy in solid neon. The species formed are identified by the
effects of isotopic substitution on their infrared spectra as well
as density functional calculations. The results show that the ground
state ScO molecule reacts with carbon dioxide to form the carbonate
complex ScCO<sub>3</sub> spontaneously on annealing. The ground state
Sc atom reacts with two carbon dioxide molecules to give the carbonate
carbonyl complex OCScCO<sub>3</sub> via the previously reported OScCO
insertion intermediate on annealing. The observation of these spontaneous
reactions is consistent with theoretical predictions that both the
Sc + 2CO<sub>2</sub> → OCScCO<sub>3</sub> and ScO + CO<sub>2</sub> → ScCO<sub>3</sub> reactions are thermodynamically
exothermic and are kinetically facile, requiring little or no activation
energy
Photoassisted Homocoupling of Methyl Iodide Mediated by Atomic Gold in Low-Temperature Neon Matrix
Infrared
spectroscopy and density functional theory calculations
showed that the gold complexes [CH<sub>3</sub>–Au–I]
and [(CH<sub>3</sub>)<sub>2</sub>–Au–I<sub>2</sub>],
in which one and two CH<sub>3</sub>I molecule(s), respectively, are
oxidatively adsorbed on the Au atoms, are formed in a solid neon matrix
via reactions between laser-ablated gold atoms and CH<sub>3</sub>I.
Global reaction route mapping calculations revealed that the heights
of the activation barriers for the sequential oxidative additions
to produce [CH<sub>3</sub>–Au–I] and [(CH<sub>3</sub>)<sub>2</sub>–Au–I<sub>2</sub>] are 0.53 and 1.00 eV,
respectively, suggesting that the reactions proceed via electronically
excited states. The reductive elimination of ethane (C<sub>2</sub>H<sub>6</sub>) from [(CH<sub>3</sub>)<sub>2</sub>–Au–I<sub>2</sub>] leaving AuI<sub>2</sub> was hindered by an activation barrier
as high as 1.22 eV but was induced by visible-light irradiation on
[(CH<sub>3</sub>)<sub>2</sub>–Au–I<sub>2</sub>]. These
results demonstrate that photoassisted homocoupling of CH<sub>3</sub>I is mediated by Au atoms via [(CH<sub>3</sub>)<sub>2</sub>–Au–I<sub>2</sub>] as an intermediate
Experimental and Theoretical Studies of the Infrared Spectra and Bonding Properties of NgBeCO<sub>3</sub> and a Comparison with NgBeO (Ng = He, Ne, Ar, Kr, Xe)
The novel neon complex NeBeCO<sub>3</sub> has been prepared in a low-temperature neon matrix via codeposition
of laser-evaporated beryllium atoms with O<sub>2</sub> + CO/Ne. Doping
by the heavier noble gas atoms argon, krypton and xenon yielded the
associated adducts NgBeCO<sub>3</sub> (Ng = Ar, Kr, Xe). The noble
gas complexes have been identified via infrared spectroscopy. Quantum
chemical calculations of NgBeCO<sub>3</sub> and NgBeO (Ng = He, Ne,
Ar, Kr, Xe) using <i>ab initio</i> methods and density functional
theory show that the Ng–BeCO<sub>3</sub> bonds are slightly
longer and weaker than the Ng–BeO bonds. The energy decomposition
analysis of the Ng–Be bonds suggests that the attractive interactions
come mainly from the Ng → BeCO<sub>3</sub> and Ng →
BeO σ donation
Infrared Photodissociation Spectroscopy of the Ni(O<sub>2</sub>)<sub><i>n</i></sub><sup>+</sup> (<i>n</i> = 2–4) Cation Complexes
The infrared spectra of mass-selected
NiÂ(O<sub>2</sub>)<sub><i>n</i></sub><sup>+</sup> (<i>n</i> = 2–4) and
their argon-tagged complexes are measured by infrared photodissociation
spectroscopy in the gas phase. The experimental spectra provide distinctive
patterns allowing the determination of their geometric and electronic
structures by comparison with the simulated vibrational spectra from
density functional theory calculations. The [NiÂ(O<sub>2</sub>)<sub>2</sub>Ar<sub>2</sub>]<sup>+</sup> cation complex was determined
to have <i>D</i><sub>2<i>h</i></sub> symmetry
involving a NiÂ(O<sub>2</sub>)<sub>2</sub><sup>+</sup> core ion with
two equivalent superoxide ligands side-on bound to a Ni<sup>3+</sup> cation center. The higher NiÂ(O<sub>2</sub>)<sub>3</sub><sup>+</sup> and NiÂ(O<sub>2</sub>)<sub>4</sub><sup>+</sup> cation complexes were
determined to have structures with a chemically bound NiÂ(O<sub>2</sub>)<sub>2</sub><sup>+</sup> core ion that is weakly coordinated by
neutral O<sub>2</sub> molecule(s)