498 IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 57, NO. 3, MARCH2008
Performance Simulation of a Quadrupole Mass Filter
Operating in the First and Third Stability Zones
Thomas J. Hogan and Stephen Taylor
Abstract—A method of computation that accurately simulates
the performance of quadrupole mass filters (QMFs) is described.
Behavior is described by determining the individual trajectories
of a large number of ions (10
8
) as they are injected into the
QMF. The effects of the ratio of circular electrode radius r to
electric field radius r0 on the performance characteristics have
been investigated for zone 1 (a ≈ 0.237 and q ≈ 0.706) and
zone 3 (a ≈ 3.16 and q ≈ 3.23) operation. We demonstrate that
performance sensitivity to the r/r0 ratio is different for zone 3
than those previously reported for zone 1. The magnitude and
variation of the “tail” in the mass spectral peak shapes that are
apparent for zone 1 is much decreased for zone 3 and does not
influence QMF resolution. Variation in ion trajectories and asso-
ciated power-spatial frequency spectra when operated in zones 1
and 3 with varying r/r0 geometrical ratios are also presented. We
demonstrate that these provide an alternative method in determin-
ing an ideal value for r/r0.
Index Terms—Mathieu stability regions, multipoles, power
frequency spectrum, quadrupole mass filter (QMF), spatial
frequencies.
I. I NTRODUCTION
Q
UADRUPOLE mass analyzers separate ions according
to their mass to charge (m/z) ratio and are a vital
component of quadrupole mass spectrometers (QMSs) that
provide the selective filtering that is necessary to separate the
constituent components of the sample under analysis. Ion trap
[1], [2], time of flight, and quadrupole mass filter (QMF) are all
types of mass analyzers providing differing performance and
operational characteristics. Attributes of the QMF have ensured
that it has been deployed in a wide range of applications from
modest residual gas analyzers to high-end mass spectrometers
for molecular analysis. The characteristics that have ensured
its widespread use include relatively simple mechanical con-
struction, simple drive requirements, acceptable power con-
sumption, and a linear mass scale. Modern process control and
scientific instrument designers are under constant pressure to
increase performance while simultaneously decreasing power
consumption and physical size. The mechanical characteristics
of the QMF make it suitable for miniaturization through the use
of microengineered mechanical system (MEMS) techniques,
providing a simultaneous reduction in operating voltage and
Manuscript received January 11, 2007; revised June 21, 2007.
The authors are with the Department of Electrical Engineering and
Electronics, University of Liverpool, L69 3GJ Liverpool, U.K. (e-mail:
t.j.hogan@liverpool.ac.uk; s.taylor@liverpool.ac.uk).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TIM.2007.911632
Fig. 1. End view of the QMF that is constructed from hyperbolic-shaped
electrodes with field radius r0 and case radius Rc.
Fig. 2. End view of the QMF that is constructed from circular electrodes with
electrode radius r, field radius r0, and case radius Rc.
power budget. The use of these techniques may require more
novel geometries to be developed. Previously reported exam-
ples of miniature mass filters include [3]–[5].
For the QMS, ideal performance is obtained when the QMF
is constructed from hyperbolic-shaped rods (Fig. 1) that are
perfectly aligned. In practice, most commercial QMFs are man-
ufactured from circular section electrodes (rods) for reasons
of cost and ease of manufacture (Fig. 2), resulting in electric
fields that deviate from the ideal. Stability zone 1 (a ≈ 0.23 and
q ≈ 0.7) is the normal operating region for most commercial
QMSs [6]. There are, however, advantages of mass spectral
peak shape, decreased evidence of low-mass “tails,” and in-
creased resolution to be gained from operation in the third
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