9 research outputs found
Model Evaluation of New Techniques for Maintaining High-NO Conditions in Oxidation Flow Reactors for the Study of OH-Initiated Atmospheric Chemistry
Oxidation flow reactors (OFRs) efficiently
produce OH radicals using low-pressure Hg-lamp emissions at λ
= 254 nm (OFR254) or both λ = 185 and 254 nm (OFR185). OFRs
under most conditions are limited to studying low-NO chemistry (where
RO<sub>2</sub> + HO<sub>2</sub> dominates RO<sub>2</sub> fate), even
though substantial amounts of initial NO may be injected. This is
due to very fast NO oxidation by high concentrations of OH, HO<sub>2</sub>, and O<sub>3</sub>. In this study, we model new techniques
for maintaining high-NO conditions in OFRs, that is, continuous NO
addition along the length of the reactor in OFR185 (OFR185-cNO), recently
proposed injection of N<sub>2</sub>O at the entrance of the reactor
in OFR254 (OFR254-iN<sub>2</sub>O), and an extension of that idea to OFR185 (OFR185-iN<sub>2</sub>O). For these techniques, we evaluate (1) fraction of conditions
dominated by RO<sub>2</sub> + NO while avoiding significant nontropospheric
photolysis and (2) fraction of conditions where reactions of precursors
with OH dominate over unwanted reactions with NO<sub>3</sub>. OFR185-iN<sub>2</sub>O
is the most practical for general high-NO experiments because it represents
the best compromise between experimental complexity and performance
upon proper usage. Short lamp distances are recommended for OFR185-iN<sub>2</sub>O
to ensure a relatively uniform radiation field. OFR185-iN<sub>2</sub>O with low O<sub>2</sub> or using Hg lamps with higher 185 nm-to-254
nm ratio can improve performance. OFR185-iN<sub>2</sub>O experiments should generally
be conducted at higher relative humidity, higher UV, lower concentration
of non-NO<sub><i>y</i></sub> external OH reactants, and
percent-level N<sub>2</sub>O. OFR185-cNO and OFR185-iN<sub>2</sub>O at optimal
NO precursor injection rate (∼2 ppb/s) or concentration (∼3%)
would have satisfactory performance in typical field studies where
ambient air is oxidized. Exposure estimation equations are provided
to aid experimental planning. This work enables improved high-NO OFR
experimental design and interpretation
Model Evaluation of New Techniques for Maintaining High-NO Conditions in Oxidation Flow Reactors for the Study of OH-Initiated Atmospheric Chemistry
Oxidation flow reactors (OFRs) efficiently
produce OH radicals using low-pressure Hg-lamp emissions at λ
= 254 nm (OFR254) or both λ = 185 and 254 nm (OFR185). OFRs
under most conditions are limited to studying low-NO chemistry (where
RO<sub>2</sub> + HO<sub>2</sub> dominates RO<sub>2</sub> fate), even
though substantial amounts of initial NO may be injected. This is
due to very fast NO oxidation by high concentrations of OH, HO<sub>2</sub>, and O<sub>3</sub>. In this study, we model new techniques
for maintaining high-NO conditions in OFRs, that is, continuous NO
addition along the length of the reactor in OFR185 (OFR185-cNO), recently
proposed injection of N<sub>2</sub>O at the entrance of the reactor
in OFR254 (OFR254-iN<sub>2</sub>O), and an extension of that idea to OFR185 (OFR185-iN<sub>2</sub>O). For these techniques, we evaluate (1) fraction of conditions
dominated by RO<sub>2</sub> + NO while avoiding significant nontropospheric
photolysis and (2) fraction of conditions where reactions of precursors
with OH dominate over unwanted reactions with NO<sub>3</sub>. OFR185-iN<sub>2</sub>O
is the most practical for general high-NO experiments because it represents
the best compromise between experimental complexity and performance
upon proper usage. Short lamp distances are recommended for OFR185-iN<sub>2</sub>O
to ensure a relatively uniform radiation field. OFR185-iN<sub>2</sub>O with low O<sub>2</sub> or using Hg lamps with higher 185 nm-to-254
nm ratio can improve performance. OFR185-iN<sub>2</sub>O experiments should generally
be conducted at higher relative humidity, higher UV, lower concentration
of non-NO<sub><i>y</i></sub> external OH reactants, and
percent-level N<sub>2</sub>O. OFR185-cNO and OFR185-iN<sub>2</sub>O at optimal
NO precursor injection rate (∼2 ppb/s) or concentration (∼3%)
would have satisfactory performance in typical field studies where
ambient air is oxidized. Exposure estimation equations are provided
to aid experimental planning. This work enables improved high-NO OFR
experimental design and interpretation
Model Evaluation of New Techniques for Maintaining High-NO Conditions in Oxidation Flow Reactors for the Study of OH-Initiated Atmospheric Chemistry
Oxidation flow reactors (OFRs) efficiently
produce OH radicals using low-pressure Hg-lamp emissions at λ
= 254 nm (OFR254) or both λ = 185 and 254 nm (OFR185). OFRs
under most conditions are limited to studying low-NO chemistry (where
RO<sub>2</sub> + HO<sub>2</sub> dominates RO<sub>2</sub> fate), even
though substantial amounts of initial NO may be injected. This is
due to very fast NO oxidation by high concentrations of OH, HO<sub>2</sub>, and O<sub>3</sub>. In this study, we model new techniques
for maintaining high-NO conditions in OFRs, that is, continuous NO
addition along the length of the reactor in OFR185 (OFR185-cNO), recently
proposed injection of N<sub>2</sub>O at the entrance of the reactor
in OFR254 (OFR254-iN<sub>2</sub>O), and an extension of that idea to OFR185 (OFR185-iN<sub>2</sub>O). For these techniques, we evaluate (1) fraction of conditions
dominated by RO<sub>2</sub> + NO while avoiding significant nontropospheric
photolysis and (2) fraction of conditions where reactions of precursors
with OH dominate over unwanted reactions with NO<sub>3</sub>. OFR185-iN<sub>2</sub>O
is the most practical for general high-NO experiments because it represents
the best compromise between experimental complexity and performance
upon proper usage. Short lamp distances are recommended for OFR185-iN<sub>2</sub>O
to ensure a relatively uniform radiation field. OFR185-iN<sub>2</sub>O with low O<sub>2</sub> or using Hg lamps with higher 185 nm-to-254
nm ratio can improve performance. OFR185-iN<sub>2</sub>O experiments should generally
be conducted at higher relative humidity, higher UV, lower concentration
of non-NO<sub><i>y</i></sub> external OH reactants, and
percent-level N<sub>2</sub>O. OFR185-cNO and OFR185-iN<sub>2</sub>O at optimal
NO precursor injection rate (∼2 ppb/s) or concentration (∼3%)
would have satisfactory performance in typical field studies where
ambient air is oxidized. Exposure estimation equations are provided
to aid experimental planning. This work enables improved high-NO OFR
experimental design and interpretation
Solvents Effects on Charge Transfer from Quantum Dots
To predict and understand the performance
of nanodevices in different environments, the influence of the solvent
must be explicitly understood. In this Communication, this important
but largely unexplored question is addressed through a comparison
of quantum dot charge transfer processes occurring in both liquid
phase and in vacuum. By comparing solution phase transient absorption
spectroscopy and gas-phase photoelectron spectroscopy, we show that
hexane, a common nonpolar solvent for quantum dots, has negligible
influence on charge transfer dynamics. Our experimental results, supported
by insights from theory, indicate that the reorganization energy of
nonpolar solvents plays a minimal role in the energy landscape of
charge transfer in quantum dot devices. Thus, this study demonstrates
that measurements conducted in nonpolar solvents can indeed provide
insight into nanodevice performance in a wide variety of environments
Laser Ablation-Aerosol Mass Spectrometry-Chemical Ionization Mass Spectrometry for Ambient Surface Imaging
Mass
spectrometry imaging is becoming an increasingly common analytical
technique due to its ability to provide spatially resolved chemical
information. Here, we report a novel imaging approach combining laser
ablation with two mass spectrometric techniques, aerosol mass spectrometry
and chemical ionization mass spectrometry, separately and in parallel.
Both mass spectrometric methods provide the fast response, rapid data
acquisition, low detection limits, and high-resolution peak separation
desirable for imaging complex samples. Additionally, the two techniques
provide complementary information with aerosol mass spectrometry providing
near universal detection of all aerosol molecules and chemical ionization
mass spectrometry with a heated inlet providing molecular-level detail
of both gases and aerosols. The two techniques operate with atmospheric
pressure interfaces and require no matrix addition for ionization,
allowing for samples to be investigated in their native state under
ambient pressure conditions. We demonstrate the ability of laser ablation-aerosol
mass spectrometry-chemical ionization mass spectrometry (LA-AMS-CIMS)
to create 2D images of both standard compounds and complex mixtures.
The results suggest that LA-AMS-CIMS, particularly when combined with
advanced data analysis methods, could have broad applications in mass
spectrometry imaging applications
Modeling the Radical Chemistry in an Oxidation Flow Reactor: Radical Formation and Recycling, Sensitivities, and the OH Exposure Estimation Equation
Oxidation
flow reactors (OFRs) containing low-pressure mercury
(Hg) lamps that emit UV light at both 185 and 254 nm (“OFR185”)
to generate OH radicals and O<sub>3</sub> are used in many areas of
atmospheric science and in pollution control devices. The widely used
potential aerosol mass (PAM) OFR was designed for studies on the formation
and oxidation of secondary organic aerosols (SOA), allowing for a
wide range of oxidant exposures and short experiment duration with
reduced wall loss effects. Although fundamental photochemical and
kinetic data applicable to these reactors are available, the radical
chemistry and its sensitivities have not been modeled in detail before;
thus, experimental verification of our understanding of this chemistry
has been very limited. To better understand the chemistry in the OFR185,
a model has been developed to simulate the formation, recycling, and
destruction of radicals and to allow the quantification of OH exposure
(OH<sub>exp</sub>) in the reactor and its sensitivities. The model
outputs of OH<sub>exp</sub> were evaluated against laboratory calibration
experiments by estimating OH<sub>exp</sub> from trace gas removal
and were shown to agree within a factor of 2. A sensitivity study
was performed to characterize the dependence of the OH<sub>exp</sub>, HO<sub>2</sub>/OH ratio, and O<sub>3</sub> and H<sub>2</sub>O<sub>2</sub> output concentrations on reactor parameters. OH<sub>exp</sub> is strongly affected by the UV photon flux, absolute humidity, reactor
residence time, and the OH reactivity (OHR) of the sampled air, and
more weakly by pressure and temperature. OH<sub>exp</sub> can be strongly
suppressed by high OHR, especially under low UV light conditions.
A OH<sub>exp</sub> estimation equation as a function of easily measurable
quantities was shown to reproduce model results within 10% (average
absolute value of the relative errors) over the whole operating range
of the reactor. OH<sub>exp</sub> from the estimation equation was
compared with measurements in several field campaigns and shows agreement
within a factor of 3. The improved understanding of the OFR185 and
quantification of OH<sub>exp</sub> resulting from this work further
establish the usefulness of such reactors for research studies, especially
where quantifying the oxidation exposure is important
Materials Properties and Solvated Electron Dynamics of Isolated Nanoparticles and Nanodroplets Probed with Ultrafast Extreme Ultraviolet Beams
We
present ultrafast photoemission measurements of isolated nanoparticles
in vacuum using extreme ultraviolet (EUV) light produced through high
harmonic generation. Surface-selective static EUV photoemission measurements
were performed on nanoparticles with a wide array of compositions,
ranging from ionic crystals to nanodroplets of organic material. We
find that the total photoelectron yield varies greatly with nanoparticle
composition and provides insight into material properties such as
the electron mean free path and effective mass. Additionally, we conduct
time-resolved photoelectron yield measurements of isolated oleylamine
nanodroplets, observing that EUV photons can create solvated electrons
in liquid nanodroplets. Using photoemission from a time-delayed 790
nm pulse, we observe that a solvated electron is produced in an excited
state and subsequently relaxes to its ground state with a lifetime
of 151 ± 31 fs. This work demonstrates that femotosecond EUV
photoemission is a versatile surface-sensitive probe of the properties
and ultrafast dynamics of isolated nanoparticles
Mapping Nanoscale Absorption of Femtosecond Laser Pulses Using Plasma Explosion Imaging
We make direct observations of localized light absorption in a single nanostructure irradiated by a strong femtosecond laser field, by developing and applying a technique that we refer to as plasma explosion imaging. By imaging the photoion momentum distribution resulting from plasma formation in a laser-irradiated nanostructure, we map the spatial location of the highly localized plasma and thereby image the nanoscale light absorption. Our method probes individual, isolated nanoparticles in vacuum, which allows us to observe how small variations in the composition, shape, and orientation of the nanostructures lead to vastly different light absorption. Here, we study four different nanoparticle samples with overall dimensions of ∼100 nm and find that each sample exhibits distinct light absorption mechanisms despite their similar size. Specifically, we observe subwavelength focusing in single NaCl crystals, symmetric absorption in TiO<sub>2</sub> aggregates, surface enhancement in dielectric particles containing a single gold nanoparticle, and interparticle hot spots in dielectric particles containing multiple smaller gold nanoparticles. These observations demonstrate how plasma explosion imaging directly reveals the diverse ways in which nanoparticles respond to strong laser fields, a process that is notoriously challenging to model because of the rapid evolution of materials properties that takes place on the femtosecond time scale as a solid nanostructure is transformed into a dense plasma
Impact of Thermal Decomposition on Thermal Desorption Instruments: Advantage of Thermogram Analysis for Quantifying Volatility Distributions of Organic Species
We
present results from a high-resolution chemical ionization time-of-flight
mass spectrometer (HRToF-CIMS), operated with two different thermal
desorption inlets, designed to characterize the gas and aerosol composition.
Data from two field campaigns at forested sites are shown. Particle
volatility distributions are estimated using three different methods:
thermograms, elemental formulas, and measured partitioning. Thermogram-based
results are consistent with those from an aerosol mass spectrometer
(AMS) with a thermal denuder, implying that thermal desorption is
reproducible across very different experimental setups. Estimated
volatilities from the detected elemental formulas are much higher
than from thermograms since many of the detected species are thermal
decomposition products rather than actual SOA molecules. We show that
up to 65% of citric acid decomposes substantially in the FIGAERO–CIMS,
with ∼20% of its mass detected as gas-phase CO<sub>2</sub>,
CO, and H<sub>2</sub>O. Once thermal decomposition effects on the
detected formulas are taken into account, formula-derived volatilities
can be reconciled with the thermogram method. The volatility distribution
estimated from partitioning measurements is very narrow, likely due
to signal-to-noise limits in the measurements. Our findings indicate
that many commonly used thermal desorption methods might lead to inaccurate
results when estimating volatilities from observed ion formulas found
in SOA. The volatility distributions from the thermogram method are
likely the closest to the real distributions