25 research outputs found
Infrared Spectroscopy of [M(CO<sub>2</sub>)<sub><i>n</i></sub>]<sup>+</sup> (M = Ca, Sr, and Ba; <i>n</i> = 1ā4) in the Gas Phase: Solvation-Induced Electron Transfer and Activation of CO<sub>2</sub>
Cationic complexes of heavy alkaline earth metal and
carbon dioxide
[M(CO2)n]+ (M =
Ca, Sr, and Ba) are produced by a laser vaporization-supersonic expansion
ion source in the gas phase and are studied by infrared photodissociation
spectroscopy in conjunction with quantum chemistry calculations. For
the n = 1 complexes, the metalāligand binding
arises primarily from the electrostatic interaction with the CO2 ligand bound to the metal (+I) center in an end-on Ī·1-O fashion. The more highly coordinated complexes [M(CO2)n]+ with n ā„ 2 are characterized to involve a [M2+(CO2ā)] core ion with the CO2ā ligand bound to the metal (+II) center in a bidentate
Ī·2-O, O manner. The activation of CO2 in
forming a bent CO2ā moiety occurs via
solvation-induced metal cation-ligand electron transfer reactions.
Bonding analyses reveal that the attractive forces between M2+ and CO2ā in the core cation come mainly
from electrostatic attraction, but the contribution of covalent orbital
interactions should not be underestimated. The atomic orbitals of
metal dications that are engaged in the orbital interactions are ns
and (n ā 1)d orbitals
Reactions of Vanadium Dioxide Molecules with Acetylene: Infrared Spectra of VO<sub>2</sub>(Ī·<sup>2</sup>āC<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>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) and
VO<sub>2</sub>(Ī·<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>(Ī·<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>(Ī·<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>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) and VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complexes are photosensitive. The
VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) complex
rearranges to the OVĀ(OH)ĀCCH molecule upon UVāvis light excitation
Infrared Photodissociation Spectroscopy and Density Functional Theory Study of Carbon Suboxide Complexes [M(CO)<sub>4</sub>(C<sub>3</sub>O<sub>2</sub>)]<sup>+</sup> (M = Fe, Co, Ni)
Infrared photodissociation spectra
are measured for mass-selected
cation complexes with a chemical formula [MC<sub>7</sub>O<sub>6</sub>]<sup>+</sup> (M = Fe, Co, Ni) formed via pulsed laser evaporation
of metal target in expansions of helium gas seeded by CO. The geometries
of the complexes are determined by comparison of the experimental
spectra with the simulated spectra from density functional calculations.
All of these complexes are identified to have [MĀ(CO)<sub>4</sub>(C<sub>3</sub>O<sub>2</sub>)]<sup>+</sup> structures involving a carbon
suboxide ligand, which binds the metal center in an Ī·<sup>1</sup> fashion. The antisymmetric CO stretching vibration of C<sub>3</sub>O<sub>2</sub> is slightly red-shifted upon coordination. The donorāacceptor
bonding interactions between C<sub>3</sub>O<sub>2</sub> and the metal
centers are analyzed using the EDA-NOCV method. The results show that
M ā C<sub>3</sub>O<sub>2</sub> Ļ donation is stronger
than the M ā C<sub>3</sub>O<sub>2</sub> Ļ back-donation
in these cation complexes
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>CrĀ(CO)<sub>2</sub>, the one-to-one CrĀ(CO<sub>2</sub>) complex and the one-to-two CrĀ(CO<sub>2</sub>)<sub>2</sub> complex as well as the CrOCrCO and OCCrCO<sub>3</sub> complexes
are also formed. The CrĀ(CO<sub>2</sub>) complex is characterized to
be side-on Ī·<sup>2</sup>-C,O-coordinated. The CrĀ(CO<sub>2</sub>)<sub>2</sub> complex is identified to involve a side-on Ī·<sup>2</sup>-C,O-coordinated CO<sub>2</sub> and an end-on Ī·<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 Ī·<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 CrĀ(CO<sub>2</sub>)<sup>+</sup> and CrĀ(CO<sub>2</sub>)<sub>2</sub><sup>+</sup> cation complexes are characterized to have linear end-on Ī·<sup>1</sup>-O-coordinated structures with blue-shifted antisymmetric
CO<sub>2</sub> stretching vibrational frequencies. The OCrCO<sup>ā</sup> anion is bent with the CrāO and CO stretching frequencies
red-shifted from those of OCrCO neutral molecule
Infrared Photodissociation Spectroscopic and Theoretical Study of Heteronuclear Transition Metal Carbonyl Cluster Cations in the Gas Phase
Heteronuclear
transition metal carbonyl cluster cations FeMĀ(CO)<sub>8</sub><sup>+</sup> (M = Co, Ni and Cu) and MCuĀ(CO)<sub>7</sub><sup>+</sup> (M
= Co and Ni) are produced via a laser vaporization supersonic cluster
ion source in the gas phase, which are each mass-selected and studied
by infrared photodissociation spectroscopy in the carbonyl stretching
frequency region. Their geometric and electronic structures are established
by comparison of the experimental spectra with those derived from
density functional theoretical calculations. The FeMĀ(CO)<sub>8</sub><sup>+</sup> (M = Co, Ni, Cu) complexes are determined to have eclipsed
(CO)<sub>5</sub>FeāMĀ(CO)<sub>3</sub><sup>+</sup> structures,
and the MCuĀ(CO)<sub>7</sub><sup>+</sup> (M = Co, Ni) ions are characterized
to have staggered (CO)<sub>4</sub>MāCuĀ(CO)<sub>3</sub><sup>+</sup> structures. Natural bonding orbital analysis indicates that
the positive charge is mainly distributed on the MĀ(CO)<sub>3</sub> fragment. The metalāmetal interaction involves an Ļ-type
(OC)<sub>4,5</sub>MāMĀ(CO)<sub>3</sub><sup>+</sup> dative bonding
Isocyanate Formation from Reactions of Early Lanthanide Metal Atoms with NO and CO in Solid Argon
The
reactions of early lanthanide metal atoms (Ce, Pr, and Nd)
with carbon monoxide and nitric oxide mixtures are studied by infrared
absorption spectroscopy in solid argon. The reaction intermediates
and products are identified via isotopic substitution as well as theoretical
frequency calculations. The results show that the reactions proceed
with the initial formation of inserted NLnO molecules, which subsequently
react with CO to form the NLnOĀ(CO) complexes on annealing. The NLnOĀ(CO)
complexes further isomerize to the more stable isocyanate OLnNCO species
under UV light excitation
Coordination and Solvation of the Au<sup>+</sup> Cation: Infrared Photodissociation Spectroscopy of Mass-Selected Au(H<sub>2</sub>O)<sub><i>n</i></sub><sup>+</sup> (<i>n</i> = 1ā8) Complexes
Gold cationāwater complexes with attached argon
atoms are
produced via a laser vaporization supersonic cluster source. The [AuĀ(H<sub>2</sub>O)<sub><i>n</i></sub>Ar<sub><i>x</i></sub>]<sup>+</sup> (<i>n</i> = 1ā8; <i>x</i> = 1 or 2) complexes are each mass selected and studied by infrared
photodissociation spectroscopy in the OH stretching frequency region
to explore the coordination and solvation structures of the Au<sup>+</sup> cation. Density functional calculations have been performed,
and the calculated vibrational spectra are compared to the experimental
spectra to identify the gas-phase structures of the AuĀ(H<sub>2</sub>O)<sub><i>n</i></sub><sup>+</sup> complexes. Confirming
previous theoretical predications, the first coordination shell of
the Au<sup>+</sup> cation contains two water molecules forming a linear
OāAu<sup>+</sup>āO arrangement; subsequent water molecules
bind to the two H<sub>2</sub>O ligands of the AuĀ(H<sub>2</sub>O)<sub>2</sub><sup>+</sup> core ion via hydrogen bond forming of the second
hydration shell, which is complete at <i>n</i> = 6. For
the complexes with <i>n</i> ā¤ 7, the experimental
spectrum can in general be assigned to the predicted global minimum
structure. However, the spectrum suggests that two or more conformers
coexist for the <i>n</i> = 8 complex, indicating that the
identification of a single global minimum becomes less important upon
increasing the number of solvating water molecules
Infrared Photodissociation Spectroscopy of Heterodinuclear IronāZinc and CobaltāZinc Carbonyl Cation Complexes
FeāZn
and CoāZn heteronuclear carbonyl cation complexes are produced
via a laser vaporization supersonic cluster source in the gas phase.
The dinuclear FeZnĀ(CO)<sub>5</sub><sup>+</sup> and CoZnĀ(CO)<sub>7</sub><sup>+</sup> cation complexes are observed to be the most intense
heterodinuclear carbonyl cation species in the mass spectra. The infrared
spectra are obtained via mass selection and infrared photodissociation
spectroscopy in the carbonyl stretching frequency region. Their geometric
and electronic structures are assigned with the support of density
functional calculations. The FeZnĀ(CO)<sub>5</sub><sup>+</sup> complex
is determined to have a (OC)<sub>5</sub>FeāZn structure with
a FeāZn half bond. The CoZnĀ(CO)<sub>7</sub><sup>+</sup> ion
is established to have a staggered (OC)<sub>4</sub>CoāZnĀ(CO)<sub>3</sub> structure involving a CoāZn Ļ single bond
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> ā OCScCO<sub>3</sub> and ScO + CO<sub>2</sub> ā ScCO<sub>3</sub> reactions are thermodynamically
exothermic and are kinetically facile, requiring little or no activation
energy