Printed circuit board
(PCB) based drift tube ion mobility spectrometers
enable the use of state-of-the-art production techniques to manufacture
compact devices with excellent performance at minimum cost. The new
PCB ion mobility spectrometer (PCB-IMS) presented here is equipped
with either a 140 MBq tritium or a 95 MBq nickel-63 ionization source
and consists of a combination of horizontally arranged 6-layer PCBs
for the drift and reaction regions and vertically arranged PCBs for
interfacing the ionization source, ion shutter, and detector. The
design allows the reproducible manufacturing and thus comparison of
different IMS topologies. Here, we investigate different ion shutters,
field-switching, Bradbury-Nielsen, and tristate and their effects
on resolving power and limits of detection considering two different
ionization region geometries and ionization sources, tritium and nickel-63.
It is shown that the high resolving power of R
P > 80 at low drift voltage of 3 kV and short drift length
of 50 mm can be achieved independent of the used ion shutter mechanism
and reaction region geometry. While the resolving power of all ion
shutters is excellent, the Bradbury-Nielsen shutter shows a pronounced
discrimination of slow ion species when using short shutter opening
times for small initial ion cloud widths, as required for high resolving
power. Thus, the intensity of the proton-bound dimer of 2-pentanone
is reduced by 30% compared to the signal intensity obtained with both
the field-switching and tristate shutter. The detection limits employing
the Bradbury-Nielsen shutter and a 50 mm reaction region as required
for nickel-63 are 58 pptv for the protonated monomer and
3.4 ppbv for the proton-bound dimer of 2-pentanone. The
detection limits achieved with the tristate shutter utilizing the
same reaction region are slightly higher for the protonated monomer
at 68 pptv, but lower for the proton-bound dimer at 2 ppbv due to the advanced ion shutter principle not discriminating
slow ions. However, the lowest detection limits of 13 pptv and 301 pptv can be achieved with the field-switching
shutter and a 2 mm reaction region, sufficient for a tritium ionization
source.