Measurements by the mass spectrometers onboard Giotto during the flyby
at comet P/Halley showed a steep increase in the ion density outside
the diamagnetic cavity at a distance of about 8000 km from the nucleus
(Balsiger et al. 1986a; Krankowsky et al. 1986). The maximum ion dens
ity was observed at a distance of 12 000 km from the nucleus rather th
an at closest approach (similar to 1000 km). This unexpected phenomeno
n, called the ion pile-up, could not be explained quantitatively so fa
r. A new physicochemical model was developed with the aim to understan
d the processes which lead to the formation of this pile-up. The semi-
empirical model is also used for interpreting the ion density data bet
ween the contact surface and a cometocentric distance of 50 000 km. A
quantitative interpretation of the measured ion densities was so far p
ossible only inside the contact surface as the physical and chemical p
rocesses are less complex there than on the outside. The model present
ed here has been applied to the water group ions (mass/charge 17, 18,
and 19 amu/e) and shows good agreement with the measurements if a neut
ral ammonia abundance of 1 to 1.5% relative to water is taken into acc
ount. The maximum in the H3O+-density at a distance of 12 000 km is th
e result of an increase in the electron temperature with increasing co
metocentric distance, which reduces the ion recombination by electrons
. As H3O+ is the most abundant ion inside 25 000 km this is also the r
eason for the enhancement of the total ion density. Although ammonia i
s destroyed with a scale-length of 4300 km, there is a significant con
tribution of NH: to the ions with mass/charge 17 amu/e in the pile-up
region. At these cometocentric distances, NH3+ results from protonatio
n of NH2 which is produced from ammonia by photodissociation and is re
latively long-lived.