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Analytical Chemistry | 2008

Atmospheric Pressure Chemical Ionization Source. 1. Ionization of Compounds in the Gas Phase

Francisco J. Andrade; Jacob T. Shelley; William C. Wetzel; Michael R. Webb; Gerardo Gamez; Steven J. Ray; Gary M. Hieftje

A novel chemical ionization source for organic mass spectrometry is introduced. This new source uses a glow discharge in the flowing afterglow mode for the generation of excited species and ions. The direct-current gas discharge is operated in helium at atmospheric pressure; typical operating voltages and currents are around 500 V and 25 mA, respectively. The species generated by this atmospheric pressure glow discharge are mixed with ambient air to generate reagent ions (mostly ionized water clusters and NO+), which are then used for the ionization of gaseous organic compounds. A wide variety of substances, both polar and nonpolar, can be ionized. The resulting mass spectra generally show the parent molecular ion (M+ or MH+) with little or no fragmentation. Proton transfer from ionized water clusters has been identified as the main ionization pathway. However, the presence of radical molecular ions (M+) for some compounds indicates that other ionization mechanisms are also involved. The analytical capabilities of this source were evaluated with a time-of-flight mass spectrometer, and preliminary characterization shows very good stability, linearity, and sensitivity. Limits of detection in the single to tens of femtomole range are reported for selected compounds.


Analytical Chemistry | 2008

Atmospheric Pressure Chemical Ionization Source. 2. Desorption−Ionization for the Direct Analysis of Solid Compounds

Francisco J. Andrade; Jacob T. Shelley; William C. Wetzel; Michael R. Webb; Gerardo Gamez; Steven J. Ray; Gary M. Hieftje

The flowing afterglow-atmospheric pressure glow discharge (APGD) ionization source described in part 1 of this study (in this issue) is applied to the direct analysis of condensed-phase samples. When either liquids or solids are exposed to the ionizing beam of the APGD, strong signals for the molecular ions of substances present on their surfaces can be detected without compromising the integrity of the solid sample structure or sample substrate. As was observed for gas-phase compounds in part 1 of this study, both polar and nonpolar substances can be ionized and detected by mass spectrometry. The parent molecular ion (or its protonated counterpart) is usually the main spectral feature, with little or no fragmentation in evidence. Preliminary quantitative results show that this approach offers very good sensitivity (detection limits in the picogram regime are reported for several test compounds in part 1 of this study) and linear response to the analyte concentration. Examples of the application of this strategy to the analysis of real-world samples, such as the direct analysis of pharmaceutical compounds or foods is provided. The ability of this source to perform spatially resolved analysis is also demonstrated. Preliminary studies of the mechanisms of the reactions involved are described.


Journal of the American Society for Mass Spectrometry | 2009

Characterization of Direct-Current Atmospheric-Pressure Discharges Useful for Ambient Desorption/Ionization Mass Spectrometry

Jacob T. Shelley; Joshua S. Wiley; George C.-Y. Chan; Gregory D. Schilling; Steven J. Ray; Gary M. Hieftje

Two relatively new ambient ionization sources, direct analysis in real time (DART) and the flowing atmospheric-pressure afterglow (FAPA), use direct current, atmospheric-pressure discharges to produce reagent ions for the direct ionization of a sample. Although at a first glance these two sources appear similar, a fundamental study reveals otherwise. Specifically, DART was found to operate with a corona-to-glow transition (C-G) discharge whereas the FAPA was found to operate with a glow-to-arc transition (G-A) discharge. The characteristics of both discharges were evaluated on the basis of four factors: reagent-ion production, response to a model analyte (ferrocene), infrared (IR) thermography of the gas used for desorption and ionization, and spatial emission characteristics. The G-A discharge produced a greater abundance and a wider variety of reagent ions than the C-G discharge. In addition, the discharges yielded different adducts and signal strengths for ferrocene. It was also found that the gas exiting the discharge chamber reached a maximum of 235 °C and 55 °C for the G-A and C-G discharges, respectively. Finally, spatially resolved emission maps of both discharges showed clear differences for N2+ and O(I). These findings demonstrate that the discharges used by FAPA and DART are fundamentally different and should have different optimal applications for ambient desorption/ionization mass spectrometry (ADI-MS).


Analytical Chemistry | 2011

Elucidation of Reaction Mechanisms Responsible for Afterglow and Reagent-Ion Formation in the Low-Temperature Plasma Probe Ambient Ionization Source

George C.-Y. Chan; Jacob T. Shelley; Joshua S. Wiley; Carsten Engelhard; Ayanna U. Jackson; R. Graham Cooks; Gary M. Hieftje

The development of ambient desorption/ionization mass spectrometry has shown promising applicability for the direct analysis of complex samples in the open, ambient atmosphere. Although numerous plasma-based ambient desorption/ionization sources have been described in the literature, little research has been presented on experimentally validating or determining the desorption and ionization mechanisms that are responsible for their performance. In the present study, established spectrochemical and plasma physics diagnostics in combination with spatially resolved optical emission profiles were applied to reveal a set of reaction mechanisms responsible for afterglow and reagent-ion formation of the Low-Temperature Plasma (LTP) probe, which is a plasma-based ionization source used in the field of ambient mass spectrometry. Within the dielectric-barrier discharge of the LTP probe, He(2)(+) is the dominant positive ion when helium is used as the plasma supporting gas. This helium dimer ion (He(2)(+)) has two important roles: First, it serves to carry energy from the discharge into the afterglow region in the open atmosphere. Second, charge transfer between He(2)(+) and atmospheric nitrogen appears to be the primary mechanism in the sampling region for the formation of N(2)(+), which is an important reagent ion as well as the key reaction intermediate for the formation of other reagent ions, such as protonated water clusters, in plasma-based ambient ionization sources. In the afterglow region of the LTP, where the sample is usually placed, a strong mismatch in the rotational temperatures of N(2)(+) (B (2)Σ(u)(+)) and OH (A (2)Σ(+)) was found; the OH rotational temperature was statistically identical to the ambient gas temperature (~300 K) whereas the N(2)(+) temperature was found to rise to 550 K toward the tail of the afterglow region. This much higher N(2)(+) temperature is due to a charge-transfer reaction between He(2)(+) and N(2), which is known to produce rotationally hot N(2)(+) (B (2)Σ(u)(+)) ions. Furthermore, it was found that one origin of excited atomic helium in the afterglow region of the LTP is from dielectronic recombination of vibrationally excited He(2)(+) ions.


Analytical Chemistry | 2008

Laser Ablation Coupled to a Flowing Atmospheric Pressure Afterglow for Ambient Mass Spectral Imaging

Jacob T. Shelley; Steven J. Ray; Gary M. Hieftje

A plasma-based ambient desorption/ionization mass spectrometry (ADI-MS) source was used to perform molecular mass spectral imaging. A small amount of sample material was ablated by focusing 266 nm laser light onto a spot. The resulting aerosol was transferred by a nitrogen stream to the flowing afterglow of a helium atmospheric pressure glow discharge ionization source; the ionized sample material was analyzed by a Leco Unique time-of-flight mass spectrometer. Two-dimensional mass spectral images were generated by scanning the laser beam across a sample surface. The total analysis time for a 6 mm (2) surface, which is limited by the washout of the ablation chamber, was less than 30 min. With this technique, a spatial resolution of approximately 20 microm has been achieved. Additionally, the laser ablation configuration was used to obtain depth information of over 2 mm with a resolution of approximately 40 microm. The combination of laser ablation with the flowing atmospheric pressure afterglow source was used to analyze several sample surfaces for a wide variety of analytes and with high sensitivity (LOD of 5 fmol for caffeine).


Analytical Chemistry | 2014

Autonomous in Situ Analysis and Real-Time Chemical Detection Using a Backpack Miniature Mass Spectrometer: Concept, Instrumentation Development, and Performance

Paul I. Hendricks; Jon K. Dalgleish; Jacob T. Shelley; Matthew A. Kirleis; Matthew T. McNicholas; Linfan Li; Tsung-Chi Chen; Chien-Hsun Chen; Jason Duncan; Frank J. Boudreau; Robert J. Noll; John P. Denton; Timothy A. Roach; Zheng Ouyang; R. Graham Cooks

A major design objective of portable mass spectrometers is the ability to perform in situ chemical analysis on target samples in their native states in the undisturbed environment. The miniature instrument described here is fully contained in a wearable backpack (10 kg) with a geometry-independent low-temperature plasma (LTP) ion source integrated into a hand-held head unit (2 kg) to allow direct surface sampling and analysis. Detection of chemical warfare agent (CWA) simulants, illicit drugs, and explosives is demonstrated at nanogram levels directly from surfaces in near real time including those that have complex geometries, those that are heat-sensitive, and those bearing complex sample matrices. The instrument consumes an average of 65 W of power and can be operated autonomously under battery power for ca. 1.5 h, including the initial pump-down of the manifold. The maximum mass-to-charge ratio is 925 Th with mass resolution of 1-2 amu full width at half-maximun (fwhm) across the mass range. Multiple stages of tandem analysis can be performed to identify individual compounds in complex mixtures. Both positive and negative ion modes are available. A graphical user interface (GUI) is available for novice users to facilitate data acquisition and real-time spectral matching.


Analytical Chemistry | 2014

Mechanisms of Real-Time, Proximal Sample Processing during Ambient Ionization Mass Spectrometry

Andre Venter; Kevin A. Douglass; Jacob T. Shelley; Gregg Hasman; Elahe Honarvar

ion. It has also been postulated that compounds can undergo direct Penning ionization with excited plasma species such as helium metastable atoms. Different classes of analytes will preferentially ionize through different mechanisms. For instance, many polar analytes will produce spectra consisting of strictly protonated molecular ions, MH + , indicating they undergo proton-transfer ionization, whereas nonpolar species, such as polycyclic aromatic hydrocarbons (PAHs), yield odd-electron molecular ions, M +· . In addition, sufficiently electronegative molecules, including halogenated or nitrated compounds, preferentially form negative ions through the Page 33 of 61 ACS Paragon Plus Environment Analytical Chemistry 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 34 mechanisms. In general, the observed ions and ionization pathways have been demonstrated to be similar to APCI and atmospheric-pressure photoionization. 163,164 Because these ionization processes rely on the formation of reagent species, differences in ionization with different plasmas can be extrapolated from background reagent-ion spectra. The DART source is an indirect plasma source which also filters any electrons and ions from the stream resulting in mostly lower energy reagent ions such as protonated water clusters, (H2O)nH + , and negative oxygen ions, O2 . 136 It was also shown that the reagent ions from DART could be altered by considerably changing source parameters, such as gas temperature and filter-electrode potentials. 165,166 In comparison, the quasidirect plasmas yield an abundance of higher-energy charge-transfer species, including N2 + , O2 + , and NO3 . 137,138 The higher energy FAPA discharge is capable of producing a significant amount of NO + . 149 The direct plasma methods can be capable of providing even higher energy reagent species, to the point where EI-like fragmentation spectra can


Analytical Chemistry | 2011

Ultrasensitive Ambient Mass Spectrometric Analysis with a Pin-to-Capillary Flowing Atmospheric-Pressure Afterglow Source

Jacob T. Shelley; Joshua S. Wiley; Gary M. Hieftje

The advent of ambient desorption/ionization mass spectrometry has resulted in a strong interest in ionization sources that are capable of direct analyte sampling and ionization. One source that has enjoyed increasing interest is the flowing atmospheric-pressure afterglow (FAPA). The FAPA has been proven capable of directly desorbing/ionizing samples in any phase (solid, liquid, or gas) and with impressive limits of detection (<100 fmol). The FAPA was also shown to be less affected by competitive-ionization matrix effects than other plasma-based sources. However, the original FAPA design exhibited substantial background levels, cluttered background spectra in the negative-ion mode, and significant oxidation of aromatic analytes, which ultimately compromised analyte identification and quantification. In the present study, a change in the FAPA configuration from a pin-to-plate to a pin-to-capillary geometry was found to vastly improve performance. Background signals in positive- and negative-ionization modes were reduced by 89% and 99%, respectively. Additionally, the capillary anode strongly reduced the amount of atomic oxygen that could cause oxidation of analytes. Temperatures of the gas stream that interacts with the sample, which heavily influences desorption capabilities, were compared between the two sources by means of IR thermography. The performance of the new FAPA configuration is evaluated through the determination of a variety of compounds in positive- and negative-ion mode, including agrochemicals and explosives. A detection limit of 4 amol was found for the direct determination of the agrochemical ametryn and appears to be spectrometer-limited. The ability to quickly screen for analytes in bulk liquid samples with the pin-to-capillary FAPA is also shown.


Biometals | 2005

Petrobactin is the primary siderophore synthesized by Bacillus anthracis str. Sterne under conditions of iron starvation

Andrew T. Koppisch; Cindy C. Browder; Amanda L. Moe; Jacob T. Shelley; Blaine A. Kinkel; Larry E. Hersman; Srinivas Iyer; Christy E. Ruggiero

The siderophores of Bacillus anthracis are critical for the pathogen’s proliferation and may be necessary for its virulence. Bacillus anthracis str. Sterne cells were cultured in iron free media and the siderophores produced were isolated and purified using a combination of XAD-2 resin, reverse-phase FPLC, and size exclusion chromatography. A combination of 1H and 13C NMR spectroscopy, UV spectroscopy and ESI-MS/MS fragmentation were used to identify the primary siderophore as petrobactin, a catecholate species containing unusual 3,4-dihydroxybenzoate moieties, previously only identified in extracts of Marinobacter hydrocarbonoclasticus. A secondary siderophore was observed and structural analysis of this species is consistent with that reported for bacillibactin, a siderophore observed in many species of bacilli. This is the first structural characterization of a siderophore from B. anthracis, as well as the first characterization of a 3,4-DHB containing catecholate in a pathogen.


Journal of Analytical Atomic Spectrometry | 2010

Ionization matrix effects in plasma-based ambient mass spectrometry sources

Jacob T. Shelley; Gary M. Hieftje

Ambient desorption/ionization mass spectrometry (ADI-MS) is an emerging field that aims to eliminate sample pretreatment and separation steps by directly desorbing and ionizing analytes from a sample surface for analysis by mass spectrometry. Although numerous applications of ADI-MS have been presented, little has been done to characterize problems caused by matrix effects. In the present study, ionization-related matrix effects were investigated for three plasma-based ADI-MS sources: the flowing atmospheric-pressure afterglow (FAPA), direct analysis in real time (DART), and the low-temperature plasma (LTP) probe. Small amounts of vapor-phase matrices were mixed with a continuous stream of gaseous analyte and introduced into each ionization source. A decrease in analyte signal upon introduction of a matrix signaled an ion-suppression event. When the matrix species had a proton affinity the same as or greater than that of the analyte, all three sources suffered analyte signal suppression, even at moderate matrix-to-analyte concentration ratios. In every case, the FAPA was the least susceptible to the ion suppression process. In contrast, when the proton affinity of the matrix species was lower than that of the analyte, no matrix effect was observed with DART, although an effect persisted for both FAPA and LTP. Indeed, matrix-to-analyte mole ratios of 10 were sufficient to entirely suppress analyte ion signals in the LTP. These findings demonstrate that matrix effects in ADI-MS are important for qualitative as well as quantitative analyses.

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Gary M. Hieftje

Indiana University Bloomington

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Andrew J. Schwartz

Indiana University Bloomington

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Francisco J. Andrade

Indiana University Bloomington

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