17 research outputs found
Infrared Spectra of M‑η<sup>2</sup>‑C<sub>2</sub>H<sub>2</sub>, HM–CCH, and HM–CCH<sup><b>–</b></sup> Prepared in Reactions of Laser-Ablated Group 3 Metal Atoms with Acetylene
The major HM–CCH and M-η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub> products are observed in the matrix infrared
spectra from reactions of laser-ablated group 3 metal atoms with acetylene,
while the vinylidene product is not detected. These results reveal
that coordination of group 3 metal atoms to the acetylene π-bond
and H-migration from C to M readily occur during codeposition and
photolysis afterward. The product absorption assigned to the La–vinylidene
complex in a previous study is reassigned to one of the absorptions
of La-η<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>···C<sub>2</sub>H<sub>2</sub>. Two strong Sc–H stretching absorptions
are assigned to the free HSc–CCH<sup>–</sup> anion,
in accord with a previous study, but a lower frequency counterpart
is reassigned to HSc–CCH<sup>–</sup> coordinated to
acetylene based on the increasing relative intensity of the low-frequency
component at higher acetylene concentration. The group 3 metals evidently
form weaker π-complexes than the group 4 metals. The addition
of an electron to HM–CCH elongates the M–H and M–C
bonds in the anionic species due to the lower ionic contributions
to the bonding
Observation and Characterization of CH<sub>3</sub>CH<sub>2</sub>–MH, (CH<sub>2</sub>)<sub>2</sub>–MH<sub>2</sub>, CH<sub>2</sub>CH–MH<sub>3</sub>, and CH<sub>3</sub>–CMH<sub>3</sub><sup>–</sup> Produced by Reactions of Group 5 Metal Atoms with Ethane
The primary products in reactions
of laser-ablated group 5 metal
atoms with ethane were identified in argon matrix IR spectra and characterized
via density functional theory computations. The second- and third-row
transition metals Nb and Ta produced insertion, metallacyclopropane,
vinyl trihydrido, and anionic ethylidyne complexes (CH<sub>3</sub>CH<sub>2</sub>–MH, (CH<sub>2</sub>)<sub>2</sub>–MH<sub>2</sub>, CH<sub>2</sub>CH–MH<sub>3</sub>, and CH<sub>3</sub>CMH<sub>3</sub><sup>–</sup>), while the first-row
transition metal V yielded only the insertion and metallacyclopropane
products. The energetically higher ethylidenes and neutral ethylidynes
(CH<sub>3</sub>CHMH<sub>2</sub> and CH<sub>3</sub>C≐MH<sub>3</sub>) were not detected. The unique
anionic ethylidynes are the most stable anionic species in the Nb
and Ta systems. Evidently back-donation from the metal center to the
C–C π* orbital is stronger than that in the group 6 metal
analogue but weaker than that in the corresponding group 4 metal complex.
The C–M bond for the Nb and Ta ethylidyne anions is a true
triple bond
Infrared Spectra of CH<sub>3</sub>–MX and CH<sub>2</sub>X–MH Prepared in Reactions of Laser-Ablated Gold, Platinum, Palladium, and Nickel Atoms with CH<sub>3</sub>Cl and CH<sub>3</sub>Br
Au,
Pt, Pd, and Ni insertion complexes have been produced in reactions
with methyl chloride and bromide. The primary products are identified
in the matrix IR spectra on the basis of deuterium shifts in the vibrational
frequencies and correlation with DFT calculated frequencies. However,
fragments of the insertion complexes and the higher oxidation state
derivatives, which have been observed in previous studies for reactions
with methane and fluoromethane, were not detected. The Pt C–H
insertion complex (CH<sub>2</sub>Cl–PtH) is also produced,
parallel to the fluorinated analogue. The observed Pt and Pd products
have highly bent CMX(H) moieties, which are traced to the unusually
high d orbital contributions from the metal atom to the C–M
and M–X(H) bonds
Infrared Spectra of CX<sub>3</sub>–AuCl and CX<sub>2</sub>–AuCl<sub>2</sub> Generated in Reactions of Laser-Ablated Gold Atoms with Chlorofluoromethanes and Carbon Tetrachloride
Laser-ablated
gold atoms have been reacted with CF<sub>3</sub>Cl, <sup>13</sup>CF<sub>3</sub>Cl, CF<sub>2</sub>Cl<sub>2</sub>, CFCl<sub>3</sub>, CCl<sub>4</sub>, and <sup>13</sup>CCl<sub>4</sub> in excess
argon during condensation, and the CX<sub>3</sub>–AuCl (X =
F, Cl) insertion products are generated. In the reactions of CFCl<sub>3</sub> and CCl<sub>4</sub> the methylidene complexes (CXCl–AuCl<sub>2</sub>) are also produced, and CFCl–AuCl<sub>2</sub> is interconvertible
with the insertion product CFCl<sub>2</sub>–AuCl upon photolysis.
The tetrachloroauric insertion and methylidene complexes are energetically
comparable and also structurally close to each other. These products
reveal that C–Cl insertion by Au readily occurs, consistent
with our previous Au investigations, and subsequent X migration also
follows in case the methylidene is energetically reachable. The C–Au
bonds of the insertion and methylidene complexes are comparable, unlike
those of the previously studied transition-metal systems, and NBO
results also show that the methylidene C–Au bond (B3LYP computed
2.04 Å) is a effectively a single bond. Evidently the gold atom
with filled 5d and 4f orbitals cannot accommodate a π system
for a methylidene-like complex without larger stabilizing/conjugating
ligands on carbon
Infrared Spectra of the Complexes Os←NCCH<sub>3</sub>, Re←NCCH<sub>3</sub>, CH<sub>3</sub>–ReNC, CH<sub>2</sub>Re(H)NC, and CHRe(H)<sub>2</sub>NC and their Mn Counterparts Prepared by Reactions of Laser-Ablated Os, Re, and Mn Atoms with Acetonitrile in Excess Argon
Acetonitrile forms primarily N-coordination complexes
(M←NCCH<sub>3</sub>) with Os and Re metal atoms, but these
metal atoms produce exclusively methylidyne complexes (HCMH<sub>2</sub>X) in similar previous reactions with small alkanes and halomethanes.
The Os complex increases on visible photolysis and dissociates partially
on UV irradiation without the generation of other new products, whereas
the Re complex converts to other products (CH<sub>3</sub>–ReNC,
CH<sub>2</sub>Re(H)NC, and CHRe(H)<sub>2</sub>NC)
on photolysis. The primary formation of the N-coordination complex
originates from its stability relative to that of the nitrile π-complex
in these systems. The agostic interaction in the methylidene complex
is apparently insignificant, and this rare observation of a methylidyne
product with Re reflects that H migration in the isocyanide system
is less favorable than those in the hydride and halide analogues.
Experiments with Mn gave weaker counterpart product absorptions
Infrared Spectra of Manganese Insertion, Vinyl, and Cyclic Complexes Prepared in Reactions of Laser-Ablated Mn Atoms with Methane, Ethane, Ethyl Chloride, and 1,2-Dichloroethane
Manganese
insertion, vinyl, and cyclic complexes are prepared in
direct reactions of excited Mn atoms with CH<sub>4</sub>, C<sub>2</sub>H<sub>6</sub>, C<sub>2</sub>H<sub>5</sub>Cl, and CH<sub>2</sub>ClCH<sub>2</sub>Cl, all with sextet ground states. The only organometallic
product observed in the reaction with methane is CH<sub>3</sub>–MnH.
The analogous insertion product C<sub>2</sub>H<sub>5</sub>–MnH
is observed with ethane, but hydrogen elimination is accompanied by
generation of the vinyl product (CH<sub>2</sub>CH–MnH). The
unusual stabilities of metallacyclic over carbene products in the
haloethane systems are in line with the previously observed group
4 metallacyclopropanes. NBO analyses reveal that the distinctively
low metal d-orbital contribution to the C–M and M–H
bonds is responsible for the linear backbones of CH<sub>3</sub>–MnH
and the group 12 metal analogues, which are similar to those of the
Grignard reagents. Systematic NBO calculations for the first-row transition-metal
CH<sub>3</sub>–MH complexes show that a low metal d-contribution
to the C–M and M–H bonds gives a linear molecular backbone
and that increasing d-character in these bonds decreases the C–M–H
angle. The stabilities of the half-filled and filled d-orbitals evidently
make the group 7 and 12 metals similar to the group 2 metals. The
tendency of increasing preference for higher oxidation state complexes
with heavier members of the group is most dramatic for the group 7
metals Mn and Re
Infrared Spectra and Density Functional Calculations for Singlet CH<sub>2</sub>SiX<sub>2</sub> and Triplet HC–SiX<sub>3</sub> and XC–SiX<sub>3</sub> Intermediates in Reactions of Laser-Ablated Silicon Atoms with Di‑, Tri‑, and Tetrahalomethanes
Reactions
of laser-ablated silicon atoms with di-, tri-, and tetrahalomethanes
in excess argon were investigated, and the products were identified
from the matrix infrared spectra, isotopic shifts, and density functional
theory energy, bond length, and frequency calculations. Dihalomethanes
produce planar singlet silenes (CH<sub>2</sub>SiX<sub>2</sub>), and tri- and tetrahalomethanes form triplet halosilyl carbenes
(HC–SiX<sub>3</sub> and XC–SiX<sub>3</sub>). The Si-bearing
molecules identified are the most stable, lowest-energy product in
the reaction systems. While the C–Si bond in the silene is
a true double bond, the C–Si bond in the carbene is a shortened
single bond enhanced by hyperconjugation of the two unpaired electrons
on C to σ*(Si–X) orbitals, which contributes stabilization
through a small amount of π-bonding and reduction of the HCSi
or XCSi angles. The C–Si bond lengths in these carbenes (1.782
Å for HC–SiF<sub>3</sub>) are between the single-bond
length in the unobserved first insertion intermediate (1.975 Å
for CHF<sub>2</sub>–SiF) and the double-bond length in the
silene (1.704 Å for CHFSiF<sub>2</sub>). The silicon
s<sup>2</sup>p<sup>2</sup> and titanium s<sup>2</sup>d<sup>2</sup> electron configurations produce similar primary products, but the
methylidyne with Ti has a bond to carbon stronger than that of the
halosilyl carbene
Matrix Infrared Spectra and Density Functional Calculations for New <i>iso</i>-Halomethanes: CHCl<sub>2</sub>–Cl, CHFCl–Cl, CFCl<sub>2</sub>–Cl, CHBr<sub>2</sub>–Br, and CBr<sub>3</sub>–Br in Solid Argon
Laser
ablation of transition metals for reactions with halocarbons
to produce new metal bearing molecules also exposed these samples
to laser plume radiation and its resulting photochemistry. Investigations
with CCl<sub>4</sub> also produced several known neutral and charged
intermediate species, including the <i>iso-</i>tetrachloromethane
CCl<sub>3</sub>–Cl observed in previous work and identified
by the Maier group. CHCl<sub>2</sub>–Cl, CHFCl–Cl, and
CFCl<sub>2</sub>–Cl, photoisomers of CHCl<sub>3</sub>, CHFCl<sub>2</sub>, and CFCl<sub>3</sub>, were also identified in matrix IR
spectra. The new C–X bonds are shorter than those of the reactants,
and the Cl atom that is weakly bonded to the residual Cl atom forms
an unusually strong C–Cl bond. NBO analysis reveals substantial
CCl double-bond character, and the weak Cl···Cl
bond is largely ionic. Therefore, the CHX<sub>2</sub>–X species
can be represented as HXCX<sup>δ+</sup>···X<sup>δ−</sup>. Ionic properties are revealed for CCl<sub>3</sub>–Cl, which has an average C–Cl bond length near
the median for the CCl<sub>3</sub> radical and cation and a natural
charge of +0.49 for the CCl<sub>3</sub> subunit. IRC computations
reproduce smooth interconversion between the reactants and products,
and the transition state is energetically close to the product, which
is consistent with its disappearance on visible irradiation
Matrix Infrared Spectra and Quantum Chemical Calculations of Ti, Zr, and Hf Dihydride Phosphinidene and Arsinidene Molecules
Laser ablated Ti,
Zr, and Hf atoms react with phosphine during
condensation in excess argon or neon at 4 K to form metal hydride
insertion phosphides (H<sub>2</sub>P-MH) and metal dihydride phosphinidenes
(HPMH<sub>2</sub>) with metal phosphorus double bonds, which
are characterized by their intense metal–hydride stretching
frequencies. Both products are formed spontaneously on annealing the
solid matrix samples, which suggests that both products are relaxed
from the initial higher energy M-PH<sub>3</sub> intermediate complex,
which is not observed. B3LYP (DFT) calculations show that these phosphinidenes
are strongly agostic with acute H–PM angles in the
60° range, even smaller than those for the analogous methylidenes
(carbenes) (CH<sub>2</sub>MH<sub>2</sub>) and in contrast
to the almost linear H-NTi subunit in the imines (H-NTiH<sub>2</sub>). Comparison of calculated agostic and terminal bond lengths
and covalent bond radii for HPTiH<sub>2</sub> with computed
bond lengths for Al<sub>2</sub>H<sub>6</sub> finds that these strong
agostic Ti–H bonds are 18% longer than single covalent bonds,
and the bridged bonds in dialane are 10% longer than the terminal
Al–H single bonds, which show that these agostic bonds can
also be considered as bridged bonds. The analogous arsinidenes (HAsMH<sub>2</sub>) have 4° smaller agostic angles and almost the same
metal–hydride stretching frequencies and double bond orders.
Calculations with fixed H–P–Ti and H–As–Ti
angles (170.0°) and <i>C</i><sub><i>s</i></sub> symmetry find that electronic energies increased by 36 and
44 kJ/mol, respectively, which provide estimates for the agostic/bridged
bonding energies
Matrix Infrared Spectra of Insertion and Metallacyclopropane Complexes [CH<sub>3</sub>CH<sub>2</sub>–MH and (CH<sub>2</sub>)<sub>2</sub>–MH<sub>2</sub>] Prepared in Reactions of Laser-Ablated Group 3 Metal Atoms with Ethane
CH<sub>3</sub>CH<sub>2</sub>–MH and (CH<sub>2</sub>)<sub>2</sub>–MH<sub>2</sub> were identified in the matrix IR spectra
from reactions of laser-ablated group 3 metal atoms with ethane, and
they were characterized via theoretical investigations. The observed
products are the most stable in the proposed reaction path. Because
of the small number of valence electrons, the group 3 metal high oxidation-state
complexes are less stable. The C–C insertion product [(CH<sub>3</sub>)<sub>2</sub>M], which was predicted to be more stable than
the observed ones, was not observed probably because of the high energy
barrier and a likely slower rate for insertion into one C–C
bond than one of six C–H bonds. The C–C bond of the
metallacyclopropanes is the shortest among the early transition-metal
analogues, and its stretching frequencies are the highest, revealing
the weakest interaction between the metal dihydride and ethylidene
groups. The undetected ethylidene is not agostic, parallel to the
previously examined methylidene