scholarly journals Response of QIT-MS to Noble Gas Isotopic Ratios in a Simulated Venus Flyby

Atmosphere ◽  
2019 ◽  
Vol 10 (5) ◽  
pp. 232 ◽  
Author(s):  
Nikolić ◽  
Madzunkov ◽  
Darrach

The primary objective of the present study is to investigate the science return of future Venus atmosphere probe mission concepts using the Quadrupole Ion Trap (QIT) Mass Spectrometer (MS) Instrument (QIT-MS-I). We demonstrate the use of Monte-Carlo simulations in determining the optimal ion trapping conditions and focus the analysis on retrieving isotope ratios of noble gases in the model sample of the Venus atmosphere. Sampling takes place at a constant velocity of ~10 km/s between 112–110 km altitude and involves the use of getter pumps to remove all chemically-active species, retaining inert noble gases. The enriched sample is leaked into passively pumped vacuum chamber where it is analyzed by the QIT-MS sensor (QIT-MS-S) for 40 minutes. The simulated mass spectrum, as recorded by the QIT-MS-S, is deconvoluted using random walk algorithm to reveal relative abundances of noble gas isotopes. The required precision and accuracy of the deconvolution method is benchmarked against the a priori known model composition of the atmospheric sample.

2004 ◽  
Vol 76 (3) ◽  
pp. 720-727 ◽  
Author(s):  
Ravi Amunugama ◽  
Jason M. Hogan ◽  
Kelly A. Newton ◽  
Scott A. McLuckey

2021 ◽  
Author(s):  
Kevin Wöhner ◽  
Toshiki Wulf ◽  
Nina Vankova ◽  
Thomas Heine

We systematically explore the stability and properties of [B<sub>12</sub>X<sub>11</sub>Ng]<sup>−</sup> adducts resulting from the capture reaction of noble gas atoms (Ng) by anionic [B<sub>12</sub>X<sub>11</sub>]<sup>−</sup> clusters in the ion trap. [B<sub>12</sub>X<sub>11</sub>]<sup>−</sup> can be obtained by stripping one X<sup>−</sup> ligand off the icosahedral <i>closo</i>-dodecaborate dianion [B<sub>12</sub>X<sub>12</sub>]<sup>2</sup><sup>−</sup>. We study the binding of the noble gas atoms He, Ne, Kr, Ar and Xe to [B<sub>12</sub>X<sub>11</sub>]<sup>−</sup> with ligands X = F, Cl, Br, I, CN. While He cannot be captured by these clusters and Ne only binds at low temperatures, the complexes with the heavier Kr, Ar and Xe show appreciable complexation energies and exceed 1 eV at room temperature in the case of [B<sub>12</sub>(CN)<sub>11</sub>Xe]<sup>−</sup>. For the latter three noble gases, we observe a significant charge transfer from the Ng to the icosahedral B<sub>12</sub> cage.


2002 ◽  
Vol 80 (12) ◽  
pp. 1433-1448 ◽  
Author(s):  
R I Thompson ◽  
T J Harmon ◽  
M G Ball

The rotating-saddle potential ball-bearing trap has long been used as a mechanical analogue to explain the operating principles of the Paul-type RF-electric-quadrupole ion trap. This paper outlines the shortcomings of this analogy, as well as explaining how and why this system remains an excellent tool for explaining ion-trap operation. The basic theory of the operating principles of the rotating-saddle trap is provided, which, unlike the Paul Trap is analytically solvable in the friction-free regime. In addition, some extensions to this theory are presented to examine such effects as friction. These results are compared with the equivalent results for Paul-Trap theory, as well as to experimental results measured with a rotating-saddle trap constructed at the University of Calgary. The technical details of this trap, an excellent tool for either lecture demonstrations or teaching laboratory experiments, are also presented, as well as some comments on building such a trap. PACS Nos.: 45.50-j, 01.50Pa, 32.80Pj


2021 ◽  
Author(s):  
Kevin Wöhner ◽  
Toshiki Wulf ◽  
Nina Vankova ◽  
Thomas Heine

We systematically explore the stability and properties of [B<sub>12</sub>X<sub>11</sub>Ng]<sup>−</sup> adducts resulting from the capture reaction of noble gas atoms (Ng) by anionic [B<sub>12</sub>X<sub>11</sub>]<sup>−</sup> clusters in the ion trap. [B<sub>12</sub>X<sub>11</sub>]<sup>−</sup> can be obtained by stripping one X<sup>−</sup> ligand off the icosahedral <i>closo</i>-dodecaborate dianion [B<sub>12</sub>X<sub>12</sub>]<sup>2</sup><sup>−</sup>. We study the binding of the noble gas atoms He, Ne, Kr, Ar and Xe to [B<sub>12</sub>X<sub>11</sub>]<sup>−</sup> with ligands X = F, Cl, Br, I, CN. While He cannot be captured by these clusters and Ne only binds at low temperatures, the complexes with the heavier Kr, Ar and Xe show appreciable complexation energies and exceed 1 eV at room temperature in the case of [B<sub>12</sub>(CN)<sub>11</sub>Xe]<sup>−</sup>. For the latter three noble gases, we observe a significant charge transfer from the Ng to the icosahedral B<sub>12</sub> cage.


2019 ◽  
Vol 34 (1) ◽  
pp. 104-117 ◽  
Author(s):  
G. Avice ◽  
A. Belousov ◽  
K. A. Farley ◽  
S. M. Madzunkov ◽  
J. Simcic ◽  
...  

A quadrupole ion trap mass spectrometer measures precisely the abundance and isotopic composition of small amounts of noble gases.


2020 ◽  
Author(s):  
Frank Maiwald ◽  
Jurij Simcic ◽  
Dragan Nikolic ◽  
Anton Belousov ◽  
Stojan Madzunkov

&lt;p&gt;The JPL Mass Spectrometer Team develops components and instruments based on a Paul quadrupole ion trap mass spectrometer (QIT-MS) for Earth and space applications. Over the past 20 years, the team has miniaturized the QIT-MS and verified its performance successfully for the International Space Station. The technology was demonstrated with the recent delivery of the first Spacecraft Atmosphere Monitor (S.A.M.) to the International Space Station (ISS).&lt;/p&gt;&lt;p&gt;The next step is to build a QIT-MS intendent to investigate the lunar exosphere via a funded ROSES 2019, DALI/NASA proposal over the next three years.&lt;/p&gt;&lt;p&gt;The QIT-MS will be the first in-situ lunar mass spectrometer capable of identifying and quantifying exosphere species (ex. H, H2, 3He, 4He, Ne, N2, O2, Ar, CH4, CO, CO2, Kr, Xe, OH, H2O) with abundance greater than 10 molecules/cm3 [1]. The combination of low mass (7.5 kg), low power (max. 30W with heater bulb on), high sensitivity (0.003 counts/cm3/sec), and ultrahigh precision (1.7 x 10&lt;sup&gt;-10&lt;/sup&gt; Torr, Kr measured continuously for 7 hours yielded a 0.6 &amp;#8240; precision on the 86Kr/84Kr ratio) will provide an unpreceded inside of the scientific processes in the lunar exosphere.&lt;/p&gt;&lt;p&gt;Other implementation approaches will be discussed, which entail the development of different frontends to expand applications for dense atmospheres (ex. Venus) or liquids (ex. ocean worlds). Most of these developments can be used to determine contaminants in the air, water, or volatile in solids.&lt;/p&gt;&lt;p&gt;[1] G. Avice, A. Belousov, K. A. Farley, S. M. Madzunkov, J. Simcic, D. Nikolic, M. R. Darrach and C. Sotin, &amp;#8220;High-precision measurements of krypton and xenon isotopes with a new static-mode quadrupole ion trap mass spectrometer,&amp;#8221; JAAS, Vol 34, January 2019&lt;/p&gt;&lt;p&gt;&amp;#160;&lt;/p&gt;&lt;p&gt;Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Dr., Pasadena, CA 91109&lt;/p&gt;&lt;p&gt;&amp;#160;&lt;/p&gt;


The Analyst ◽  
2019 ◽  
Vol 144 (18) ◽  
pp. 5608-5616
Author(s):  
Abdil Özdemir ◽  
Jung-Lee Lin ◽  
Mustafa Gülfen ◽  
Chun-Jen Hsiao ◽  
Chung-Hsuan Chen

In this work, we report a new design of a charge detection quadrupole ion trap mass spectrometer (QIT-MS) for the analysis of micro-sized dry inorganic and bioparticles including red blood cells (RBCs) and different sizes of MCF-7 breast cancer cells.


2021 ◽  
Vol 217 (1) ◽  
Author(s):  
J. Simcic ◽  
D. Nikolić ◽  
A. Belousov ◽  
D. Atkinson ◽  
C. Lee ◽  
...  

AbstractTo date, a variety of different types of mass spectrometers have been utilized on missions to study the composition of atmospheres of solar system bodies, including Venus, Mars, Jupiter, Titan, the moon, and several comets. With the increasing interest in future small probe missions, mass spectrometers need to become even more versatile, lightweight, compact, and sensitive.For in situ exploration of ice giant atmospheres, the highest priority composition measurements are helium and the other noble gases, noble gas isotopes, including 3He/4He, and other key isotopes like D/H. Other important but lower priority composition measurements include abundances of volatiles C, N, S, and P; isotopes 13C/12C, 15N/14N, 18O/17O/16O; and disequilibrium species PH3, CO, AsH3, GeH4, and SiH4. Required measurement accuracies are largely defined by the accuracies achieved by the Galileo (Jupiter) probe Neutral Mass Spectrometer and Helium Abundance Detectors, and current measurement accuracies of solar abundances.An inherent challenge of planetary entry probe mass spectrometers is the introduction of material to be sampled (gas, solid, or liquid) into the instrument interior, which operates at a vacuum level. Atmospheric entry probe mass spectrometers typically require a specially designed sample inlet system, which ideally provides highly choked, nearly constant mass-flow intake over a large range of ambient pressures. An ice giant descent probe would have to operate for 1-2 hours over a range of atmospheric pressures, possibly covering 2 or more orders of magnitude, from the tropopause near 100 mbar to at least 10 bars, in an atmospheric layer of depth beneath the tropopause of about 120 km at Neptune and about 150 km at Uranus.The Jet Propulsion Laboratory’s Quadrupole Ion Trap Mass Spectrometer (QITMS) is being developed to achieve all of these requirements. A compact, wireless instrument with a mass of only 7.5 kg, and a volume of 7 liters (7U), the JPL QITMS is currently the smallest flight mass spectrometer available for possible use on planetary descent probes as well as small bodies, including comet landers and surface sample return missions. The QITMS is capable of making measurements of all required constituents in the mass range of 1–600 atomic mass units (u) at a typical speed of 50 mass spectra per second, with a sensitivity of up to $10^{13}$ 10 13  counts/mbar/sec and mass resolution of $m/\Delta m=18000$ m / Δ m = 18000 at m/q = 40. (Throughout this paper we use the unit of m/q = u/e for the mass-to-charge ratio, where atomic mass unit and elementary charge are $1~\text{u} = 1.66\times 10^{-27}~\text{kg}$ 1 u = 1.66 × 10 − 27 kg and $1\text{e} = 1.6\times 10^{-19}$ 1 e = 1.6 × 10 − 19 C, respectively.) The QITMS features a novel MEMS-based inlet system driven by a piezoelectric actuator that continuously regulates gas flow at inlet pressures of up to 100 bar.In this paper, we present an overview of the QITMS capabilities, including instrument design and characteristics of the inlet system, as well as the most recent results from laboratory measurements in different modes of operation, especially suitable for ice giant atmospheres exploration.


The Analyst ◽  
2021 ◽  
Author(s):  
Fuxing Xu ◽  
Weimin Wang ◽  
Bingjun Qian ◽  
Liuyu Jin ◽  
Chuanfan Ding

The effective electric field radius is a fundamental parameter of ion trap which has great influence on ion trapping capability, signal intensity, mass range and some other properties of ion...


2000 ◽  
Vol 194 (2-3) ◽  
pp. 225-234 ◽  
Author(s):  
Carsten Weil ◽  
J.Mitchell Wells ◽  
H Wollnik ◽  
R.Graham Cooks

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