PFI-PEPICO takes advantage
of the multibunch time structure of the ALS storage ring (512 ns of
synchrotron radiation followed by a 144-ns dark gap). The ALS photons
excite C3H7Cl
molecules to energies in the vicinity of the ion dissociation threshold.
While promptly produced electrons and ions are extracted by a small
electric field, some neutral molecules in high-n Rydberg states remain.
These need just a small energy boost to become ionized. That energy
is provided by a pulsed electrical field (pulsed-field ionization,
or PFI) during the 144-ns dark gap. The resultant photoelectrons provide
the start signal for time-of-flight measurements of the corresponding
photoions (photoelectron-photoion coincidence, or PEPICO). By measuring
the relative abundance of C3H7Cl+
vs. C3H7+
over a range of photon energies, the researchers were able to determine
very precisely at what energy the abundance of C3H7Cl+
goes to zero (i.e., where C3H7Cl+
dissociates completely into C3H7+
and Cl).
Left:
Time-of-flight distributions for C3H7Cl+
and C3H7+
at selected photon energies.
Right: Relative abundance of C3H7Cl+
vs. C3H7+
in the vicinity of the ion dissociation threshold, or "appearance
energy" (AE) of C3H7+
at 0 K.
|
This dissociation threshold
energy represents the energy change that occurs when the parent molecule
(C3H7Cl) splits into the products
(C3H7+ and Cl) or vice versa
(in which case this energy is called the heat of formation). Because the
heats of formation of C3H7Cl
and Cl are well known, the heat of formation of C3H7+
can now be determined with an accuracy limited by the error in the heat
of formation of C3H7Cl. Then,
because C3H7+ is made up of
C3H6 (propene) and H+
(a proton), the heats of formation of C3H7+
(from this work) and H+ (well established) yield
the change in energy involved in attaching a proton to propene (i.e.,
its proton affinity). As mentioned above, propene provides one of the
absolute reference points for the scale of relative proton affinities.
Similar measurements and calculations
were performed for ethylene (C2H4),
another "anchor" molecule for the proton affinity scale. These more accurate
heats of formation led to proton affinities of 742.3 kJ/mol for propene
and 682.0 kJ/mol for ethylene, in good agreement with the latest theoretical
calculations and about 8 kJ/mol lower than the previously accepted standard
values. An example of the effect of these measurements for selected molecules
having proton affinity values between 700 and 800 kJ/mole is shown above.
Research conducted by T. Baer (University of North Carolina at Chapel
Hill), Y. Song and C.Y. Ng (Ames Laboratory), J. Liu and W. Chen (Berkeley
Lab).
Research funding: Office of Basic Energy Sciences (BES), U.S. Department
of Energy (DOE). Operation of the ALS is supported by BES.
Publications about this experiment: T. Baer, Y. Song, C.Y. Ng, J. Liu,
W. Chen, "The Heat of Formation of 2-C3H7+
and Proton Affinity of C3H6 Determined by Pulsed Field Ionization-Photoelectron
Photoion Coincidence Spectroscopy," J. Phys. Chem. A 104(9), 1959 (2000).
T. Baer, Y. Song, J. Liu, W. Chen, C.Y. Ng, "Pulsed field ionization-photoelectron
photoion coincidence spectroscopy with synchrotron radiation: The heat
of formation of the C2H5+ ion," Faraday Discuss. 115, 137 (2000).
ALSNews Vol.
169, January 31, 2001 |