Ions stored in an electrodynamic ion trap can be forced
from the
center of the ion trap to regions of higher radio frequency (RF) electric
fields by exposing them to a dipolar DC (DDC) potential applied across
opposing electrodes. Such ions absorb power from the trapping RF field,
resulting in increased ripple motion at the frequency of the trapping
RF. When a bath gas is present, ions undergo energetic collisions
that result in “RF-heating” sufficient to induce fragmentation.
DDC is therefore a broad-band (i.e., mass-to-charge-independent) means
for collisional activation in ion traps with added bath gas. Under
appropriate conditions, the internal energy distribution of an ion
population undergoing dissociation can be approximated with an effective
temperature, Teff. In such cases, it is possible to determine
thermal activation parameters, such as Arrhenius activation energies
and A-factors, by measuring dissociation kinetics. In this work, the
well-studied thermometer ion, protonated leucine enkephalin, was subjected
to DDC activation under rapid energy exchange conditions and in two
separate bath gases, N2 and Ar, to measure Teff as a function of the ratio of DDC and RF voltages. As a result,
an empirically derived calibration was generated to link experimental
conditions to Teff. It was also possible to quantitatively
evaluate a model described by Tolmachev et al. that can be used to
predict Teff. It was found that the model, which was derived
under the assumption of an atomic bath gas, accurately predicts Teff when Ar was used as the bath gas but overestimates Teff when N2 was the bath gas. Adjustment of the
Tolmachev et al. model for a diatomic gas resulted in an underestimate
of Teff. Thus, use of an atomic gas can provide accurate
activation parameters, while an empirical correction factor should
be used to generate activation parameters using N2.