Method Development and Evaluation of the infiTOF Time-of-Flight
Mass Spectrometer for On-site Helium Isotopes Analysis
*Kirk Richard Jensen
1
, Hirochika Sumino
2
, Toshinobu Hondo
1,3
, Michisato Toyoda
1
1. Project Research Center for Fundamental Sciences, Graduate School of Science, Osaka University, Osaka, Japan, 2.
Department of Basic Science, Graduate School of Arts and Sciences, University of Tokyo, Tokyo, Japan, 3.
MS-Cheminformatics, LLC, Inabe-gun, Mie, Japan
Active volcanoes can cause devastating destruction, and as such, it would be desirable to be able to
predict these disasters before their occurrence. One possibility involves measuring helium, which has two
stable isotopes,
3
He and
4
He. The ratio of these two isotopes in geochemical reservoirs such as the
atmosphere, ocean, crust, and mantle are different depending on the balance of primordial (relatively
enriched in
3
He compared to the atmosphere) and radiogenic (predominantly
4
He) helium. The
3
He/
4
He
ratios of hot springs and groundwater around a volcano have values between magmatic (up to 1.1 x 10
-5
or more) and crustal (less than 1 x 10
^-7
) helium isotope ratios, the latter resulting from dissolution of
radiogenic helium into groundwater from crustal rocks. When magma becomes active, the
3
He/
4
He ratios
of nearby hot springs/groundwater may increase as the relative contribution of magmatic helium is
expected to be higher. Such
3
He/
4
He increases preceding volcanic eruptions have been reported for El
Hierro Island, Canary (Padrón et al., Geology, 41, 2013) and Ontake, Japan (Sano et al., Scientific Reports,
5, 2014). The
3
He/
4
He ratio of hot springs/groundwater around a volcano has great potential for
monitoring magmatic activity. Currently, magnetic-sector mass spectrometry (MS) is used to measure
3
He/
4
He, however, adequate mass resolution to discriminate
3
He from HD and a high-vacuum line to purify
and separate helium from other gaseous species are required to measure
3
He/
4
He ratios because helium
concentration is generally quite low (1-100 ppmv in gas samples or 1-100 ppt in water samples).
Moreover,
3
He accounts for only 0.1-10 ppm of total helium. For these reasons, helium isotope analysis is
limited to a suitable laboratory, and on-site, real-time monitoring of
3
He/
4
He around a volcano is almost
impossible.
The “infiTOF” is a small, portable, time-of-flight (TOF) mass spectrometer capable of high mass
resolution and high mass accuracy. The applicability of infiTOF for helium isotope monitoring was
investigated by using software-based ion counting and a high-speed digitizer (commonly used in modern
TOF instruments instead of a traditional time-digital-converter (TDC)), to measure extremely low-level
signals. This configuration is advantageous compared to a TDC-based system because the averaged
profile waveform can be used to monitor the overall spectrum, including high concentration ions. The
concentration ratio of
3
He compared to
4
He in the expected sample is in the range of 10
-6
to 10
-8
, and
because of this large difference, they can not be monitored together without saturating the detector.
Therefore,
4
He
2+
was measured as a quantitative reference for
4
He
+
. The
3
He
+
/
4
He
2+
ratio of a sample was
measured using the infiTOF MS by counting ion peaks from each TOF trigger waveform. A
3
He standard
was measured to verify the
3
He peak and measure mass accuracy, which was observed with an error of
4.30 x 10
-5
Da. The
3
He
+
/
4
He
2+
ratio was measured for three different helium gas cylinders by infiTOF.
Mass accuracy for
4
He
2+
and
3
He
+
was also determined for sample cylinders with errors of 3.00 x 10
-8
Da
and 2.25 x 10
-4
Da respectively. All cylinders were also measured by magnetic sector MS at University of
Tokyo using standard helium gas HESJ (Helium standard of Japan, Matsuda et al., Geochem. J., 36, 2002).
Using one cylinder as a secondary standard, the
3
He
+
/
4
He
2+
ratios for the other cylinders were determined
using infiTOF measurements, which were then compared to the magnetic sector MS measurements and
found to be in agreement with less than 5% error. Mass drift was also investigated and found to be less
than 50 x 10
-6
Da over ten hours. Results indicate that this method is accurate, stable, and has enough
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