A Miniature Cylindrical Quadrupole Ion Trap: Simulation and Experiment

A recently developed prototype mobile laboratory mass spectrometer, incorporating an atmospheric pressure ionization (API) interface, is described. This system takes advantage of the small size, lower voltage requirements, and tandem MS abilities of the cylindrical ion trap mass analyzer. The prototype API MS uses small, low-power pumps to fit into a 0.1-m 3 self-contained package weighing <45 kg. This instrument has been adapted to allow rapid interfacing to electrospray ionization, desorption electrospray ionization, and direct analysis in real-time sources. Initial data indicate that these techniques provide rapid detection and identification of compounds for quality control, homeland security, and forensic applications. In addition, this instrument is self-contained and compact, making it ideally extensible to mobile laboratory and field analyses. Initial MS and MS/MS data for analyses of drugs, food, and explosives are presented herein. O ver the past 15 years, efforts toward implementing mass spectrometry (MS) in the field have steadily grown with particular focus on environmental, forensic, defense, and security applications [I, 2]. Many of the previously developed fieldable MS instruments use gas chromatography (GC-MS) because of the high degree of confidence obtained using GC retention times and electron ionization (EI) mass spectral matching [3][4][5][6]. The specificity of GC-MS comes at the expense of time, with individual analyses often taking in excess of 10 min (not including sample preparation). Reducing the amount of time required for chemical identification requires separation-free MS. In the absence of chromatography, tandem MS (MS/MS) improves confidence for the identification of individual components in mixtures [7]. With spectral acquisition rates > 1 Hz, atmospheric pressure ionization (API) techniques such as electrospray ionization (ESI), desorption electro spray (DESI), and direct analysis in real time (DART), a fieldable API MS system capable of MS/MS is of high value to environmental, forensic, defense, and force protection agencies. There have been few attempts to construct fieldable MS instruments with an API interface to date [8][9][10][11] because of the difficulty of displacing the gas load of the atmospheric inlet.The cylindrical ion trap (CIT)-a simplified geometry of the hyperbolic quadrupole ion trap capable of Address reprint requests to Dr. Mitch Wells, Griffin Analytical Technologies, LLC, R&D, 3000 Kent Avenue, West Lafayette, IN 47906, USA. E-mail: mitch.wells@icxt.com performing MS n analyses-has been shown to be amenable to miniaturization [12][13][14] while maintaining benchtop-quality performance characteristics. The miniaturized CIT enables a smaller vacuum system with smaller pumps that consume less power, providing a fieldable instrument. Although GC-MS instruments currently dominate the portable mass spectrometry industry, estimates indicate that the confidence for molecule identification by MS/MS is about that provided with GC-MS (when combining MS information w...

Section: Performing Msmentioning

confidence: 99%

Implementation of DART and DESI ionization on a fieldable mass spectrometer

Wells¹,

Roth²,

Keil³

et al. 2008

“…In contrast to TOFs, linear quadrupoles, and magnetic sectors [19], ion traps enjoy the ability to perform tandem mass spectrometry with a single mass analyzer [20]. The simplified geometry of a cylindrical ion trap in comparison to 3D ion traps has led to a significant research investment in the miniaturization of ion traps [21][22][23][24][25][26] and micro-fabricated ion trap arrays [27][28][29]. Lammert [30,31] and Austin [32][33][34] have studied toroidal ion traps of various geometries in an attempt to expand the quantitative dynamic range of ion traps in miniature and portable instruments.…”

Section: Introductionmentioning

confidence: 99%

Performance Evaluation of a Loeb-Eiber Mass Filter at 1 Torr

Hoffmann

Feng

Pedder³

et al. 2014

Abstract. The Loeb-Eiber mass filter is best operated at relatively high pressures-such as 1 Torr-where collisional dampening of ions up to the mass filter thermalizes the ions' kinetic energy, which is a requirement for effective filtering. The inter-electrode gaps of~8 μm require rf amplitudes on the order of 0-5 V p-p at approximately 50 MHz to achieve mass filtering up to m/z 40. Mass filtering between the 25-μm diameter wires, therefore, takes place on time frames less than the collision frequency at~1 Torr. The low power and high pressure capabilities of the Loeb-Eiber mass filter make it ideally suited for miniaturization, where power and space are a premium. In the present work, a Loeb-Eiber mass filter was constructed using commercial silicon-on-insulator (SOI) microfabrication techniques. Ions transmitting through the chip-based Loeb-Eiber mass filter were characterized in real time using a traditional linear quadrupole mass analyzer in series with the Loeb-Eiber mass filter. The new hybrid instrument has enabled us to verify several important claims regarding the operation of the Loeb-Eiber mass filter: (1) that ions can be effectively filtered at~1 Torr, (2) that for ions of a fixed mass-to-charge ratio, the ion transmission current decreases linearly with increasing rf amplitude on the Loeb-Eiber mass filter, (3) that the cutoff voltage at which all ions of a particular m/z value are effectively blocked is linearly related to mass-to-charge, and (4) that square waveforms can filter ions more effectively than sinusoidal waveforms for a given peak-to-peak rf amplitude.

“…While there have been numerous attempts to make small analyzers, not all can reasonably be called miniature [1]. However, quadrupole mass filters [2-6] and various types of ion traps [7][8][9] with characteristic dimensions of the order of a few millimeters or less have been demonstrated. The size and weight contribution to a complete mass spectrometer system is not the only benefit of a miniaturized quadrupole mass filter.…”

mentioning

confidence: 99%

Comparison of ion coupling strategies for a microengineered quadrupole mass filter

Wright¹,

Syms

O'Prey³

et al. 2009

The limitations of conventional machining and assembly techniques require that designs for quadrupole mass analyzers with rod diameters less than a millimeter are not merely scale versions of larger instruments. We show how silicon planar processing techniques and microelectromechanical systems (MEMS) design concepts can be used to incorporate complex features into the construction of a miniature quadrupole mass filter chip that could not easily be achieved using other microengineering approaches. Three designs for the entrance and exit to the filter consistent with the chosen materials and techniques have been evaluated. The differences between these seemingly similar structures have a significant effect on the performance. Although one of the designs results in severe attenuation of transmission with increasing mass, the other two can be scanned to m/z ϭ 400 without any corruption of the mass spectrum. At m/z ϭ 219, the variation in the transmission of the three designs was found to be approximately four orders of magnitude. A maximum resolution of M/⌬M ϭ 87 at 10% peak height has been achieved at m/z ϭ 219 with a filter operated at 6 MHz and constructed using rods measuring ( nterest in the miniaturization of mass analyzers has been growing rapidly in recent years, largely driven by the need for compact, lightweight systems for use in environmental, security, and space applications. While there have been numerous attempts to make small analyzers, not all can reasonably be called miniature [1]. However, quadrupole mass filters [2-6] and various types of ion traps [7][8][9] with characteristic dimensions of the order of a few millimeters or less have been demonstrated. The size and weight contribution to a complete mass spectrometer system is not the only benefit of a miniaturized quadrupole mass filter. The rf amplitude required to achieve a particular mass range increases with the square of the rod radius. Hence, the rf supplies for miniature filters can be smaller and require less power than those needed for larger filters. More importantly, smaller pumps may be used, as the short path length of ions in the filter means that a higher pressure can be tolerated. Although this paper is focused on miniaturization of the filter, reports on the development of other miniaturized components that might be incorporated into a system, such as ion sources, gauges, and pumps can be found elsewhere [10 -12].The factors that determine the size of a miniature quadrupole mass filter are the required signal level, the accuracy of the construction technique, and the number of rf cycles needed to achieve the desired resolution. Clearly, as the size of the entrance aperture decreases, there will be an inevitable loss of signal, although some of this can be recovered through the use of an array [2,4]. There is a well-known correlation [13] between the fractional geometrical error and ultimate resolution. Hence, one fundamental limitation is set by the accuracy of the fabrication technique and the minimum acceptable resolution. Si...