6 research outputs found
<i>Ab Initio</i> Study of Decay Dynamics of 1‑Nitronaphthalene Initiated from the S<sub>2</sub>(ππ* + n<sub>NO</sub>π*) State
Irradiation of nitro-PAHs
in solution at ambient conditions leads
to formation of its lowest excited triplet, dissociation intermediates
nitrogen oxide (NO<sup>•</sup>) and aryloxy radical (Ar–O<sup>•</sup>). Experimental and theoretical studies demonstrated
that Franck–Condon excited singlet state S<sub>FC</sub>(ππ*)
to a receiver, higher-energy triplet state T<sub>n</sub>(nπ*)
controlled the ultrafast population of the triplet state and, hence,
the slight fluorescence yield of nitronaphthalenes. However, the detailed
information about the curve-crossings of potential energy surfaces
and the major channels for forming T<sub>1</sub> species and Ar–O<sup>•</sup> radical were unclear. Here, by using the CASSCF//CASPT2
method, an efficient decay channel is revealed: S<sub>2‑FC‑1NN</sub> → S<sub>2‑MIN‑1NN</sub> or S<sub>2</sub>T<sub>3‑MIN‑1NN</sub> → T<sub>3‑MIN‑1NN</sub> or T<sub>3</sub>T<sub>2‑MIN‑1NN</sub>→ T<sub>2‑MIN‑1NN</sub> or T<sub>2</sub>T<sub>1‑MIN‑1NN</sub> → T<sub>1‑MIN‑1NN</sub>. This explains the
high yield of T<sub>1–1NN</sub> species and minor yield of
Ar–O<sup>•</sup> and NO<sup>•</sup> radicals.
The calculation results suggest the bifurcation processes take place
predominantly after the internal conversion to the T<sub>1–1NN</sub> state via T<sub>2</sub>T<sub>1‑MIN‑1NN</sub>, one
leads to T<sub>1‑MIN‑1NN</sub>, while the other to T<sub>1‑MIN‑ISO</sub> to produce Ar–O<sup>•</sup> and NO<sup>•</sup> radicals
Excited State Proton Transfer Dynamics of Thioacetamide in S<sub>2</sub>(ππ*) State: Resonance Raman Spectroscopic and Quantum Mechanical Calculations Study
The photophysics and photochemistry
of thioacetamide (CH<sub>3</sub>CSNH<sub>2</sub>) after excitation
to the S<sub>2</sub> electronic
state were investigated by using resonance Raman spectroscopy in conjunction
with the complete active space self-consistent field (CASSCF) method
and density functional theory (DFT) calculations. The A-band resonance
Raman spectra in acetonitrile, methanol, and water were obtained at
299.1, 282.4, 266.0, 252.7, and 245.9 nm excitation wavelengths to
probe the structural dynamics of thioacetamide in the S<sub>2</sub> state. CASSCF calculations were done to determine the transition
energies and structures of the lower-lying excited states, the conical
intersection points CIÂ(S<sub>2</sub>/S<sub>1</sub>) and CIÂ(S<sub>1</sub>/S<sub>0</sub>), and intersystem crossing points. The structural
dynamics of thioacetamide in the S<sub>2</sub> state was revealed
to be along eight Franck–Condon active vibrational modes ν<sub>15</sub>, ν<sub>11</sub>, ν<sub>14</sub>, ν<sub>10</sub>, ν<sub>8</sub>, ν<sub>12</sub>, ν<sub>18</sub>, and ν<sub>19</sub>, mostly in the CC/CS/CN stretches
and the CNH<sub>8</sub>,<sub>9</sub>/CCH<sub>5,6,7</sub>/CCN/CCS in-plane
bends as indicated by the corresponding normal mode descriptions.
The S<sub>2</sub> → S<sub>1</sub> decay process via the S<sub>2</sub>/S<sub>1</sub> conical intersection point as the major channel
were excluded. The thione–thiol photoisomerization reaction
mechanism of thioacetamide via the S<sub>2,FC</sub> → S′<sub>1,min</sub> excited state proton transfer (ESPT) reaction channel
was proposed
Intermolecular Hydrogen Abstraction from Hydroxy Group and Alkyl by T<sub>1</sub>(ππ*) of 1‑Chloro-4-nitronaphthalene
Nanosecond
transient absorption and theoretical calculations have
been used to investigate the intermolecular hydrogen abstractions
from alcohols and 1-naphthol by the lowest excited triplet (T<sub>1</sub>) of 1-chloro-4-nitronaphthalene upon excitation of the compound
in organic solvents. The hydrogen abstraction of T<sub>1</sub> from
hydroxy group of 1-naphthol takes place through an electron transfer
followed by a proton transfer through hydrogen bonding interaction
with rate constants of ∼10<sup>9</sup> M<sup>–1</sup> s<sup>–1</sup>. Hydrogen-bonding is crucial in this process,
indicated by the observation of a half reduction for T<sub>1</sub> yield when increasing the concentration of 1-naphthol. The hydrogen
abstraction in this way can be decelerated by increasing solvent polarity
and hydrogen-bonding donor ability. The T<sub>1</sub> of 1-chloro-4-nitronaphthalene
can undergo one-step H atom abstraction from alkyl hydrogen in alcoholic
solvents, with rate constants of ∼10<sup>4</sup> M<sup>–1</sup> s<sup>–1</sup>, and produce radical intermediates with the
absorption maximum at 368 nm. DFT calculation results indicate both
oxygens of the nitro group are active sites for hydrogen abstraction,
and the difference of activation barriers for formation of two radical
isomers is only 1.0 kcal/mol
UV and Resonance Raman Spectroscopic and Theoretical Studies on the Solvent-Dependent Ground and Excited-State Thione → Thiol Tautomerization of 4,6-Dimethyl-2-mercaptopyrimidine (DMMP)
The vibrational spectra
of 4,6-dimethyl-2-mercaptopyrimidine (DMMP)
in acetonitrile, methanol, and water were assigned by resonance Raman
spectroscopy through a combination of Fourier-transform infrared spectroscopy
(FT-IR), FT-Raman UV–vis spectroscopy, and density functional
theoretical (DFT) calculations. The FT-Raman spectra show that the
neat solid DMMP is formed as a dimer due to intermolecular hydrogen
bonding. In methanol and water, however, the majority of the Raman
spectra were assigned to the vibrational modes of DMMPÂ(solvent)<sub><i>n</i></sub> (<i>n</i> = 1–4) clusters
containing NH···O hydrogen bonds. The intermolecular
NH···O hydrogen bond interactions, which are key constituents
of the stable DMMP thione structure, revealed significant structural
differences in acetonitrile, methanol, and water. In addition, UV-induced
hydrogen transfer isomeric reactions between the thione and thiol
forms of DMMP were detected in water and acetonitrile. DFT calculations
indicate that the observed thione → thiol tautomerization should
occur easily in lower excited states in acetonitrile and water
Direct Observation of 4‑Phenoxyphenylnitrenium Ion: A Transient Absorption and Transient Resonance Raman Study
Femtosecond (fs) and nanosecond (ns)
transient absorption (TA)
and single pulse transient resonance Raman spectroscopic investigation
of the intermediates after laser photolysis of 4-phenoxyphenyl azide
in acetonitrile and mixed aqueous solution is reported. fs-TA results
show that the singlet 4-phenoxyphenylnitrene was produced immediately
after photolysis of the azide. Then, the singlet nitrene underwent
intersystem crossing (ISC) and ring expansion to generate triplet
nitrene and ketenimine in acetonitrile with <i>t</i> = 346
ps or protonation in mixed aqueous solution with <i>t</i> = 37 ps, respectively, a little slower than the counterparts of
the methoxy one (108 and 5.4 ps for ISC and protonation processes,
respectively). The transient Raman spectrum combined density functional
theory (DFT) calculation predicting the structure and vibrational
frequencies suggested that phenoxyphenylnitrenium ion has a comparable
quinoidal character to that of methoxy- and ethoxy-phenylnitrenium
ions. All of these results indicated that the phenoxy substitution
has some impact on the reactivity of phenylnitrene but a slight influence
on the structure of phenylnitrenium ion
Excited State Structures and Decay Dynamics of 1,3-Dimethyluracils in Solutions: Resonance Raman and Quantum Mechanical Calculation Study
The
resonance Raman spectroscopic study of the excited state structural
dynamics of 1,3-dimethyluracil (DMU), 5-bromo-1,3-dimethyluracil (5BrDMU),
uracil, and thymine in water and acetonitrile were reported. Density
functional theory calculations were carried out to help elucidate
the ultraviolet electronic transitions associated with the A-, and
B-band absorptions and the vibrational assignments of the resonance
Raman spectra. The effect of the methylation at N1, N3 and C5 sites
of pyrimidine ring on the structural dynamics of uracils in different
solvents were explored on the basis of the resonance Raman intensity
patterns. The relative resonance Raman intensities of DMU and 5BrDMU
are computed at the B3LYP-TD level. Huge discrepancies between the
experimental resonance Raman intensities and the B3LYP-TD predicted
ones were observed. The underlying mechanism was briefly discussed.
The decay channel through the S<sub>1</sub>(<sup>1</sup>nπ*)/S<sub>2</sub>(<sup>1</sup>ππ*) conical intersection and the
S<sub>1</sub>(<sup>1</sup>nπ*)/T<sub>1</sub>(<sup>3</sup>ππ*)
intersystem crossing were revealed by using the CASSCFÂ(8,7)/6-31GÂ(d)
level of theory calculations