chemical physics of discharges - Argonne National Laboratory

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variable from 0 - 100 volts. There are no provisions for measuring pressure,
temperature, or ionizing current in the ion source. The ions are focused and
accelerated to 50 - 100 volts, and mass analyzed by a quadrupole mass filter with a
length of 10.0 inches and an ro of 0.27 inches. Mass scanning is accomplished by
varying the RF and DC voltages to the quadrupole. The resolution of the quadrupole
is electronically variable. The ions are then accelerated to 600 volts and detected
by a Bendix Channeltron continuous electron multiplier.
Because of the absence of slits in the mass spectrometer, the lrelatively open
nature of the ion source, and the high sensitivity of the detector, it is necessary
to reduce the background from scattered electrons reaching the detector. This is
accomplished in two ways:
the electrons but not the ions; and second, by pulsing the electron beam. The
ionizing beam is pulsed at 10 kc by applying a 40 volt pulse to the first lens of
the electron beam. The beam ''on'' time is 10 microseconds. After a delay of 5
microseconds, the second pulser sends a one volt pulse to turn on the transistor-
ized "AND" gate for 20 - 30 microseconds.
first, by establishing a weak magnetic field to deflect
Only those pulses which arrive at the
gate during this interval are sent on to the ratemeter. At the voltages used, most
of the electrons arrive at the detector vithin one or two microseconds; the flight
time of the negative ions, however, is of the order of 10 - 20 microseconds. Thus,
the signal to the ratemeter is primarily due to ions, with a drastic reduction in
the electron background. The output of the ratemeter is plotted versus the DC
voltage on the quadrupole with an XY recorder. A signal of five ions per second
can readily be observed. A typical plot, shown in Fig. 2, is the lover portion of
the mass spectrum of the negative ions of pentaborane.
All the boron hydride samples were purified by distillation in a vacuum
system. The diborane was trapped out at -154OC. The tetraborane was purified in
three steps: pumping off hydrogen and diborane while trapped at -130, passing
through a trap at -95 to condense the pentaborane and the higher boron hydrides,
and finally condensing at -196. The pentaborane was similarly purified: pumping
off diborane and tetraborane at -98, passing through a trap at -79, and final trapping
at -196.
Results and Discussion
The results are shown in the bar graph in Fig. 3. The narrow bars represent
peaks which have been multiplied by a factor of ten. All measurements are for 70
volt ionizing electrons. The monoisotopic mass spectrum was computed assuming the
natural BlO/B11 distribution of 20/80, and also assuming that there was no isotope
effect in loss of hydrogen from B10 versus B11. In nearly all cases, the Ykak
heights from which the monoisotopic spectra were calculated were an average of at
least three measurements, with separate measurements in agreement within 10%. In
calculating the monoisotopic spectrum, the system is "over-determined," :.e., there
are more equations than there are unknowns. This provides a means of checking the
internal consistency of the results. For every case except tvo, the self-consistency
deviation was less than 2%, and in all cases less than 10%. On the basis Of
these consi_derations, relative intensities within a group of peaks, e.g., BgHg ,
B5He , B5H7 , etc., should be accurate to 2 10%.
In comparing peaks between
different groups, however, it is more difficult to assign limits of error, for the
spectrometer may favor the observation of low masses over high masses in certain
cases. One can observe this "discrimination" in the positive ion spectra, and it
appears to be primarily a function of the resolution of the quadrupole. It is
possible, however, that the continuous electron multiplier and the ion source also
mass discriminate, perhaps differently for positive and negative ions.
Since the
signal from the multiplier is analyzed as pulses rather than current, mass discrim-
ination by the detector should be minimized. The exit holes in our ion source are
rather large, and it would be expected that discrimination here would also be
negligible. Thus, if it is assumed that the discrimination effects are the same
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