4 research outputs found
Theoretical Study on Reaction Mechanism of Ground-State Cyano Radical with 1,3-Butadiene: Prospect of Pyridine Formation
The reaction of ground-state cyano
radicals, CNÂ(X<sup>2</sup>ÎŁ<sup>+</sup>), with the simplest
polyene, 1,3-butadiene (C<sub>4</sub>H<sub>6</sub>(X<sup>1</sup>A<sub>g</sub>)), is investigated to explore
probable routes and feasibility to form pyridine at ultralow temperatures.
The isomerization and dissociation channels for each of the seven
initial collision complexes are characterized by utilizing the unrestricted
B3LYP/cc-pVTZ and the CCSDÂ(T)/cc-pVTZ calculations. With facilitation
of RRKM rate constants, through ab initio paths composed of 7 collision
complexes, 331 intermediates, 62 hydrogen atom, 71 hydrogen molecule,
and 3 hydrogen cyanide dissociated products, the most probable paths
at collision energies up to 10 kcal/mol, and thus the reaction mechanism,
are determined. Subsequently, the corresponding rate equations are
solved that the concentration evolutions of collision complexes, intermediates,
and products versus time are obtained. As a result, the final products
and yields are determined. The low-energy routes for the formation
of most thermodynamically stable product, pyridine, are identified.
This study, however, predicts that seven collision complexes would
produce predominately 1-cyano-1,3-butadiene, CH<sub>2</sub>CHÂCHCHÂCN
(<b>p2</b>) plus atomic hydrogen via the collision complex <b>c1</b>(CH<sub>2</sub>CHÂCHCÂH<sub>2</sub>CN) and intermediate <b>i2</b>(CH<sub>2</sub>CHÂCH<sub>2</sub>CHÂCN), with a
very minor amount of pyridine. Our scheme also effectively excludes
the presence of 2-cyano-1,3-butadiene, which has energy near-degenerate
to 1-cyano-1,3-butadiene, as supported by experimental findings
Silicon Quantum Dot-Based Fluorescence Turn-On Metal Ion Sensors in Live Cells
Multiple
sensor systems are designed by varying aza-crown ether moiety in silicon
quantum dots (SiQDs) for detecting individual Mg<sup>2+</sup>, Ca<sup>2+</sup>, and Mn<sup>2+</sup> metal ions with significant selectivity
and sensitivity. The detection limit of Mg<sup>2+</sup>, Ca<sup>2+</sup>, and Mn<sup>2+</sup> can reach 1.81, 3.15, and 0.47 ÎĽM, respectively.
Upon excitation of the SiQDs which are coordinated with aza-crown
ethers, the photoinduced electron transfer (PET) takes place from
aza-crown ether moiety to the valence band of SiQDs core such that
the reduced probability of electron–hole recombination may
diminish the subsequent fluorescence. The fluorescence suppression
caused by such PET effect will be relieved after selective metal ion
is added. The charge-electron binding force between the metal ion
and aza-crown ether hinders the PET and thereby restores the fluorescence
of SiQDs. The design of sensor system is based on the fluorescence “turn-on”
of SiQDs while in search of the appropriate metal ion. For practical
application, the sensing capabilities of metal ions in the live cells
are performed and the confocal image results reveal their promising
applicability as an effective and nontoxic metal ion sensor
Combined Crossed Molecular Beam and ab Initio Investigation of the Multichannel Reaction of Boron Monoxide (BO; X<sup>2</sup>Σ<sup>+</sup>) with Propylene (CH<sub>3</sub>CHCH<sub>2</sub>; X<sup>1</sup>A′): Competing Atomic Hydrogen and Methyl Loss Pathways
The reaction dynamics of boron monoxide
(<sup>11</sup>BO; X<sup>2</sup>ÎŁ<sup>+</sup>) with propylene
(CH<sub>3</sub>CHCH<sub>2</sub>; X<sup>1</sup>A′) were investigated
under single collision
conditions at a collision energy of 22.5 ± 1.3 kJ mol<sup>–1</sup>. The crossed molecular beam investigation combined with <i>ab initio</i> electronic structure and statistical (RRKM) calculations
reveals that the reaction follows indirect scattering dynamics and
proceeds via the barrierless addition of boron monoxide radical with
its radical center located at the boron atom. This addition takes
place to either the terminal carbon atom (C1) and/or the central carbon
atom (C2) of propylene reactant forming <sup>11</sup>BOC<sub>3</sub>H<sub>6</sub> intermediate(s). The long-lived <sup>11</sup>BOC<sub>3</sub>H<sub>6</sub> doublet intermediate(s) underwent unimolecular
decomposition involving at least three competing reaction mechanisms
via an atomic hydrogen loss from the vinyl group, an atomic hydrogen
loss from the methyl group, and a methyl group elimination to form <i>cis</i>-/<i>trans</i>-1-propenyl-oxo-borane (CH<sub>3</sub>CHCH<sup>11</sup>BO), 3-propenyl-oxo-borane (CH<sub>2</sub>CHCH<sub>2</sub><sup>11</sup>BO), and ethenyl-oxo-borane (CH<sub>2</sub>CH<sup>11</sup>BO), respectively. Utilizing partially deuterated
propylene (CD<sub>3</sub>CHCH<sub>2</sub> and CH<sub>3</sub>CDCD<sub>2</sub>), we reveal that the loss of a vinyl hydrogen atom is the
dominant hydrogen elimination pathway (85 ± 10%) forming <i>cis</i>-/<i>trans</i>-1-propenyl-oxo-borane, compared
to the loss of a methyl hydrogen atom (15 ± 10%) leading to 3-propenyl-oxo-borane.
The branching ratios for an atomic hydrogen loss from the vinyl group,
an atomic hydrogen loss from the methyl group, and a methyl group
loss are experimentally derived to be 26 ± 8%:5 ± 3%:69
± 15%, respectively; these data correlate nicely with the branching
ratios calculated via RRKM theory of 19%:5%:75%, respectively
Combined Crossed Molecular Beam and Ab Initio Investigation of the Reaction of Boron Monoxide (BO; X<sup>2</sup>ÎŁ<sup>+</sup>) with 1,3-Butadiene (CH<sub>2</sub>CHCHCH<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>) and Its Deuterated Counterparts
The reactions of the boron monoxide
(<sup>11</sup>BO; X<sup>2</sup>ÎŁ<sup>+</sup>) radical with 1,3-butadiene
(CH<sub>2</sub>CHCHCH<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>) and
its partially deuterated
counterparts, 1,3-butadiene-<i>d</i><sub>2</sub> (CH<sub>2</sub>CDCDCH<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>) and 1,3-butadiene-<i>d</i><sub>4</sub> (CD<sub>2</sub>CHCHCD<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>), were investigated under single collision conditions
exploiting a crossed molecular beams machine. The experimental data
were combined with the state-of-the-art ab initio electronic structure
calculations and statistical RRKM calculations to investigate the
underlying chemical reaction dynamics and reaction mechanisms computationally.
Our investigations revealed that the reaction followed indirect scattering
dynamics through the formation of <sup>11</sup>BOC<sub>4</sub>H<sub>6</sub> doublet radical intermediates via the barrierless addition
of the <sup>11</sup>BO radical to the terminal carbon atom (C1/C4)
and/or the central carbon atom (C2/C3) of 1,3-butadiene. The resulting
long-lived <sup>11</sup>BOC<sub>4</sub>H<sub>6</sub> intermediate(s)
underwent isomerization and/or unimolecular decomposition involving
eventually at least two distinct atomic hydrogen loss pathways to
1,3-butadienyl-1-oxoboranes (CH<sub>2</sub>CHCHCH<sup>11</sup>BO)
and 1,3-butadienyl-2-oxoboranes (CH<sub>2</sub>C (<sup>11</sup>BO)ÂCHCH<sub>2</sub>) in overall exoergic reactions via tight exit transition
states. Utilizing partially deuterated 1,3-butadiene-<i>d</i><sub>2</sub> and -<i>d</i><sub>4</sub>, we revealed that
the hydrogen loss from the methylene moiety (CH<sub>2</sub>) dominated
with 70 ± 10% compared to an atomic hydrogen loss from the methylidyne
group (CH) of only 30 ± 10%; these data agree nicely with the
theoretically predicted branching ratio of 80% versus 19%