13 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 Photodissociation Spectroscopic and Theoretical Study of Homoleptic Dinuclear Chromium Carbonyl Cluster Cations with a Linear Bridging Carbonyl Group
Infrared spectra of mass-selected homoleptic dinuclear
chromium
carbonyl cluster cations Cr<sub>2</sub>(CO)<sub><i>n</i></sub><sup>+</sup> with <i>n</i> = 7–9 are measured
via infrared photodissociation spectroscopy in the carbonyl stretching
frequency region in the gas phase. The structures are established
by comparison of the experimental spectra with the simulated spectra
derived from density functional calculations. The Cr<sub>2</sub>(CO)<sub><i>n</i></sub><sup>+</sup> cluster cations are characterized
to have the (OC)<sub>5</sub>Cr–C–O–CrÂ(CO)<sub><i>n</i>−6</sub><sup>+</sup> structures with a linear
bridging carbonyl group bonded to one chromium atom through its carbon
atom and to the other chromium atom through its oxygen atom. The cluster
cations all have a sextet ground state with the positive charge and
the unpaired electrons located on the CrÂ(CO)<sub><i>n</i>−6</sub> moiety. The formation of the linear bridging structures
without Cr–Cr bonding can be rationalized that chromium forms
strong Cr–CO bonds but weak Cr–Cr bonds
Infrared Photodissociation Spectroscopy of Mass Selected Homoleptic Copper Carbonyl Cluster Cations in the Gas Phase
Infrared spectra of mass-selected
homoleptic copper carbonyl cluster
cations including dinuclear Cu<sub>2</sub>(CO)<sub>6</sub><sup>+</sup> and Cu<sub>2</sub>(CO)<sub>7</sub><sup>+</sup>, trinuclear Cu<sub>3</sub>(CO)<sub>7</sub><sup>+</sup>, Cu<sub>3</sub>(CO)<sub>8</sub><sup>+</sup>, and Cu<sub>3</sub>(CO)<sub>9</sub><sup>+</sup>, and
tetranuclear Cu<sub>4</sub>(CO)<sub>8</sub><sup>+</sup> are measured
via infrared photodissociation spectroscopy in the carbonyl stretching
frequency region. The structures are established by comparison of
the experimental spectra with simulated spectra derived from density
functional calculations. The Cu<sub>2</sub>(CO)<sub>6</sub><sup>+</sup> cation is characterized to have an unbridged <i>D</i><sub>3<i>d</i></sub> structure with a Cu–Cu half bond.
The Cu<sub>2</sub>(CO)<sub>7</sub><sup>+</sup> cation is determined
to be a weakly bound complex involving a Cu<sub>2</sub>(CO)<sub>6</sub><sup>+</sup> core ion. The trinuclear Cu<sub>3</sub>(CO)<sub>7</sub><sup>+</sup> and Cu<sub>3</sub>(CO)<sub>8</sub><sup>+</sup> cluster
cations are determined to have triangle Cu<sub>3</sub> core structures
with <i>C</i><sub>2</sub> symmetry involving two CuÂ(CO)<sub>3</sub> groups and one CuÂ(CO)<sub><i>x</i></sub> group
(<i>x</i> = 1 or 2). In contrast, the trinuclear Cu<sub>3</sub>(CO)<sub>9</sub><sup>+</sup> cluster cation is determined
to have an open chain-like (OC)<sub>3</sub>Cu–CuÂ(CO)<sub>3</sub>–CuÂ(CO)<sub>3</sub> structure. The tetranuclear Cu<sub>4</sub>(CO)<sub>8</sub><sup>+</sup> cluster cation is characterized to have
a tetrahedral Cu<sub>4</sub><sup>+</sup> core structure with all carbonyl
groups terminally bonded
Carbonyl Bonding on Oxophilic Metal Centers: Infrared Photodissociation Spectroscopy of Mononuclear and Dinuclear Titanium Carbonyl Cation Complexes
Mononuclear and dinuclear titanium carbonyl cation complexes
including
TiÂ(CO)<sub>6</sub><sup>+</sup>, TiÂ(CO)<sub>7</sub><sup>+</sup>, TiOÂ(CO)<sub>5</sub><sup>+</sup>, Ti<sub>2</sub>(CO)<sub>9</sub><sup>+</sup> and
Ti<sub>2</sub>OÂ(CO)<sub>9</sub><sup>+</sup> are produced via a laser
vaporization supersonic cluster source. The ions are mass selected
in a tandem time-of-flight mass spectrometer and studied with infrared
photodissociation spectroscopy in the CO stretching frequency region.
The structures are established by comparison of the experimental spectra
with simulated spectra derived from density functional calculations.
Only one IR band is observed for the 15-electron TiÂ(CO)<sub>6</sub><sup>+</sup> cation, which is characterized to have an octahedral <i>O</i><sub><i>h</i></sub> structure. The TiÂ(CO)<sub>7</sub><sup>+</sup> cation is determined to be a weakly bound complex
involving a TiÂ(CO)<sub>6</sub><sup>+</sup> core ion instead of the
seventh coordinated ion. The TiOÂ(CO)<sub>5</sub><sup>+</sup> cation
has a completed coordination sphere with a C<sub>4v</sub> structure.
The Ti<sub>2</sub>(CO)<sub>9</sub><sup>+</sup> cation is determined
to have a doublet <i>C</i><sub><i>s</i></sub> structure
with two four-electron donor side-on bridging CO groups and one semibridging
CO group. The Ti<sub>2</sub>OÂ(CO)<sub>9</sub><sup>+</sup> cation has
a doublet <i>C</i><sub><i>s</i></sub> structure
involving a planar cyclic Ti<sub>2</sub>OÂ(η<sup>2</sup>-μ-CO)
core with a four electron donor side-on bridging CO. Bonding analysis
indicates that the Ti<sub>2</sub>(CO)<sub>9</sub><sup>+</sup> and
Ti<sub>2</sub>OÂ(CO)<sub>9</sub><sup>+</sup> cations each have a Ti–Ti
single bond. The results suggest that metal–metal multiple
bonding is not favorable, and the oxophilic titanium centers failed
to satisfy the 18-electron configuration in these metal carbonyl complexes
Summary statistics of the ESTs generated from the German cockroach through pyrosequencing.
<p>Summary statistics of the ESTs generated from the German cockroach through pyrosequencing.</p
Genes related to important physiological functions.
<p>Genes related to important physiological functions.</p
Phylogeny of the OBPs (A) and CSPs (B) from the German cockroach and their homologs.
<p>The unrooted consensus trees with 1000 bootstrap replicates are generated in MEGA6 <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0106932#pone.0106932-Tamura1" target="_blank">[39]</a> using the neighbor-joining method. The tree is drawn to scale, with branch lengths in the same units as those of the evolutionary distances used to infer the phylogenetic tree. All positions containing gaps and missing data are eliminated. GenBank accession numbers and species names of the sequences used here are shown in the phylogenetic trees. German cockroach OBPs and CSPs (marked by •) are in bolds.</p
Length distribution of clean reads (A) produced by 454 pyrosequencing and the assembled unigenes (B).
<p>Length distribution of clean reads (A) produced by 454 pyrosequencing and the assembled unigenes (B).</p
Phylogeny of two gustatory receptor genes from the German cockroach.
<p>Unigenes c5791 (A) and c rep c30027 (B) are highlighted in bolds and triangles (â–´).</p