21 research outputs found
Double Imaging Photoelectron Photoion Coincidence Sheds New Light on the Dissociation of State-Selected CH<sub>3</sub>F<sup>+</sup> Ions
The
vacuum ultraviolet (VUV) photoionization and dissociative photoionization
of methyl fluoride (CH<sub>3</sub>F) in the 12.2–19.8 eV energy
range were investigated by using synchrotron radiation coupled to
a double imaging photoelectron photoion coincidence (i<sup>2</sup>PEPICO) spectrometer. The production of several fragment ions including
CH<sub>2</sub>F<sup>+</sup>, CHF<sup>+</sup>, CH<sub>3</sub><sup>+</sup>, and CH<sub>2</sub><sup>+</sup> as a function of state and internal
energy of CH<sub>3</sub>F<sup>+</sup> ions was identified and analyzed,
with their individual appearance energies measured through threshold
photoelectron spectroscopy. Dynamical information was inferred from
electron and ion kinetic energy correlation diagrams measured at chosen
fixed photon energies. The detailed mechanisms governing the dissociation
of state-selected CH<sub>3</sub>F<sup>+</sup> ions prepared in the
X<sup>2</sup>E, A<sup>2</sup>A<sub>1</sub>, and B<sup>2</sup>E low-lying
electronic states as well as outside the Franck–Condon region
have been inferred based on the present experimental results and existing
theoretical calculations. Both the CH<sub>2</sub>F<sup>+</sup> and
CH<sub>3</sub><sup>+</sup> primary fragment ions have three different
channels of production from different electronic states of CH<sub>3</sub>F<sup>+</sup>. The spin–orbit splitting states of the
F fragment, <sup>2</sup>P<sub>3/2</sub> and <sup>2</sup>P<sub>1/2</sub>, in the CH<sub>3</sub><sup>+</sup> + F dissociation channels were
assigned and adiabatically correlate to the X<sup>2</sup>E ground
state and the A<sup>2</sup>A<sub>1</sub> electronic state, respectively,
with the aid of previous theoretical results. The CH<sub>3</sub>F<sup>+</sup> ions in the high energy part of the X<sup>2</sup>E ground
state are unstable and statistically dissociate to the CH<sub>2</sub>F<sup>+</sup>(1<sup>1</sup>A<sub>1</sub>) and HÂ(<sup>2</sup>S) fragments
along the potential energy curve of the X<sup>2</sup>E state. The
A<sup>2</sup>A<sub>1</sub> electronic state is a repulsive state and
exclusively dissociates to the CH<sub>3</sub><sup>+</sup>(1<sup>1</sup>A<sub>1</sub>′) and FÂ(<sup>2</sup>P<sub>1/2</sub>) fragments.
In addition, the CH<sub>2</sub>F<sup>+</sup>, CHF<sup>+</sup>, CH<sub>3</sub><sup>+</sup>, and CH<sub>2</sub><sup>+</sup> fragment ions
are also produced in the B<sup>2</sup>E state and in the Franck–Condon
gap by indirect processes, such as internal conversion or dissociative
autoionization
Quenching of the Electrochemiluminescence of Tris(2,2′-bipyridine)ruthenium(II)/Tri‑<i>n</i>‑propylamine by Pristine Carbon Nanotube and Its Application to Quantitative Detection of DNA
In this study, we describe the quenching of electrochemiluminescence
(ECL) of trisÂ(2,2′-bipyridine)-rutheniumÂ(II)Â(RuÂ(bpy)<sub>3</sub><sup>2+</sup>)/tri-<i>n</i>-propylamineÂ(TPA) at pristine
multiwall carbon nanotube (MWNT) modified glassy carbon (GC) electrode.
Even though the faradic current of the RuÂ(bpy)<sub>3</sub><sup>2+</sup>/TPA system and the oxidation of TPA obtained at pristine MWNT-modified
GC electrode is enhanced compared with those at the bare GC electrode,
the intensity of ECL produced at MWNT electrode is smaller than that
at GC electrode. For testing the possible reason of quenching, a comparison
of ECL behavior of RuÂ(bpy)<sub>3</sub><sup>2+</sup>/TPA at pristine
MWNT and acid-treated, heat-treated, and polyethylene glycol (PEG)-wrapped
MWNT-modified GC electrode is studied. The results demonstrate that
the oxygen-containing groups at the surface of MWNT and the intrinsic
electron properties of MWNT are considered to be the major reason
for the suppression of ECL. The comparison also demonstrates that
this quenching is related to the distance between MWNT and RuÂ(bpy)<sub>3</sub><sup>2+</sup>/TPA. Utilizing this essential quenching mechanism,
a new signal-on DNA hybridization assay is proposed on the basis of
the MWNT modified electrode, where single-stranded DNA (ssDNA) labeled
with RuÂ(bpy)<sub>3</sub><sup>2+</sup> derivatives probe (Ru-ssDNA)
at the distal end is covalently attached onto the MWNT electrode.
ECL signal is quenched where Ru-ssDNA is self-organized on the surface
of MWNT electrode; however, the quenched ECL signal returns in case
of the presence of complementary ssDNA. The developed approach for
sequence-specific DNA detection has good selectivity, sensitivity,
and signal-to-background ratio. Therefore, the quenching of the ECL
of RuÂ(bpy)<sub>3</sub><sup>2+</sup>/TPA system by the pristine MWNT
can be an excellent platform for nucleic acid studies and molecular
sensing
Hazard ratios for cause-specific mortality according joint categories of body mass index.
<p>Hazard ratios (95% CI) indicates the risk of body mass index (BMI) <18 kg/m<sup>2</sup> compared with the risk in all the other BMI groups. The adjusted model includes sex and age. The fully adjusted model includes smoking, drinking, physical activity, systolic blood pressure, history of cardiovascular disorders, serum lipid disturbance, diabetes mellitus and antihypertensive drug treatment additionally.</p>*<p>p<0.05,</p>§<p>p<0.01,</p>¶<p>p<0.001.</p
Multivariable-adjusted hazard ratios (95% CI) for all causes mortality, cardiovascular mortality and non-cardiovascular mortality across eight groups of body mass index (BMI).
<p>The hazard ratio express the risk in the BMI group compared with the average risk in the whole study population, which were adjusted for sex, age, smoking, drinking, physical activity, systolic blood pressure, history of cardiovascular disorders, serum lipid disturbance, diabetes mellitus and antihypertensive drug treatment.</p
Baseline characteristics of the community hypertensive patients by category of body-mass index.
<p>Data are No. (%) or mean±SD. SBP and DBP indicate systolic and diastolic blood pressures. P values are for the difference among the eight groups. P values less than 0.05 are shown in bold and italics.</p
Cumulative incidence of all causes mortality, cardiovascular mortality and non-cardiovascular mortality across eight groups of body mass index (BMI).
<p>G1 to G8 indicate ascending BMI groups. Cutoff points were 18, 20, 22, 24, 26, 28,30 kg/m<sup>2</sup>.</p
Multivariable adjusted hazard ratios for all causes mortality, cardiovascular mortality and non-cardiovascular mortality of body mass index (BMI) <18 kg/m<sup>2</sup> in subgroup analysis.
<p>The Cox regression model were adjusted for sex, age, smoking, drinking, physical activity, systolic blood pressure, history of cardiovascular disorders, serum lipid disturbance, diabetes mellitus and antihypertensive drug treatment additionally. Subgroups of age were determined according to quintiles.</p>*<p>p<0.05,</p>§<p>p<0.01,</p>¶<p>p<0.001.</p
Cl-Loss Dynamics of Vinyl Chloride Cations in the B<sup>2</sup>A″ State: Role of the C<sup>2</sup>A′ State
The
dissociative photoionization of vinyl chloride (C<sub>2</sub>H<sub>3</sub>Cl) in the 11.0–14.2 eV photon energy range was
investigated using threshold photoelectron photoion coincidence (TPEPICO)
velocity map imaging. Three electronic states, namely, A<sup>2</sup>A′, B<sup>2</sup>A″, and C<sup>2</sup>A′, of
the C<sub>2</sub>H<sub>3</sub>Cl<sup>+</sup> cation were prepared,
and their dissociation dynamics were investigated. A unique fragment
ion, C<sub>2</sub>H<sub>3</sub><sup>+</sup>, was observed within the
excitation energy range. TPEPICO three-dimensional time-sliced velocity
map images of C<sub>2</sub>H<sub>3</sub><sup>+</sup> provided the
kinetic energy release distributions (KERD) and anisotropy parameters
in dissociation of internal-energy-selected C<sub>2</sub>H<sub>3</sub>Cl<sup>+</sup> cations. At 13.14 eV, the total KERD showed a bimodal
distribution consisting of Boltzmann- and Gaussian-type components,
indicating a competition between statistical and non-statistical dissociation
mechanisms. An additional Gaussian-type component was found in the
KERD at 13.65 eV, a center of which was located at a lower kinetic
energy. The overall dissociative photoionization mechanisms of C<sub>2</sub>H<sub>3</sub>Cl<sup>+</sup> in the B<sup>2</sup>A″
and C<sup>2</sup>A′ states are proposed based on time-dependent
density functional theory calculations of the Cl-loss potential energy
curves. Our results highlight the inconsistency of previous conclusions
on the dissociation mechanism of C<sub>2</sub>H<sub>3</sub>Cl<sup>+</sup>
Associations of Lp-PLA<sub>2</sub> mass with intracranial and extracranial arterial stenosis.
<p>OR, odds ratio. Model I adjusted for age and sex. Model II adjusted for age, sex, BMI, hypertension duration, current smoking and drinking status, diabetes, LDL, HDL, plasma glucose, mean arterial pressure, heart rate, neutrophil account, urine albumin creatinine ratio, serum creatinine, anti-hypertensive treatment, and statin use. The odds ratio expressed the risk in the ICAS and ECAS group compared with the non-stenosis group. Isolated ECAS, extracranial arterial stenosis only; Isolated ICAS, intracranial arterial stenosis only; COMB, combined extra- and intracranial arterial stenosis. Complex ICAS, intracranial arterial stenosis no matter how was the extracranial arteries; Hypertension duration, neutrophil account, serum creatinine, urine albumin creatinine ratio and Lp-PLA<sub>2</sub> are log-transformed.</p><p>Associations of Lp-PLA<sub>2</sub> mass with intracranial and extracranial arterial stenosis.</p
Prevalence of moderate to severe ECAS and ICAS (%) (A) and distribution of ICAS vessels (B) according to tertiles of Lp-PLA<sub>2</sub>.
<p>ECAS, extracranial arterial stenosis; ICAS, intracranial arterial stenosis; Lp-PLA2, Lipoprotein-associated phospholipase A<sub><b>2</b></sub>.</p