Antihydrogen (

) contains a
positron and an antiproton and
is the simplest atom that is made up of antimatter. Two
large experimental groups, involving collaborators in several
countries,
have been working hard for several years on the construction at CERN
of the experimental apparatus needed to trap and store

at very
low
temperatures. The projects that they are working on are called
ATHENA and ATRAP. For a review of the background to research on

,
see Charlton
et al., Physics
Reports 241, 65 (1994), Holzscheiter and
Charlton, Rep. Prog. Phys. 62, 1 (1999) and Gabrielse, Adv. At. Mol.
Phys.
45, 1 (2001).

In the summer of 2002, the experimentalists working on the ATHENA
project
were successful in preparing about 50,000

atoms at a temperature
of about 15 K. See Nature 419, 456 (2002).

was subsequently
prepared by the ATRAP project. See Phys. Rev. Lett. 89. 213401,233401
(2002).
This is a very exciting development. It should lead on to experiments
to study the properties of

. Of particular interest are tests
of
the CPT invariance of quantum field theory and also of Einstein's
principle
of equivalence, which is the cornerstone of the general theory of
relativity.
To be able to carry out these experiments, it will be necessary to trap
and
store

at temperatures below 1 K.
The first work we carried out on

was the calculation of
an upper
bound
to the critical distance below which a proton and an antiproton are
unable
to bind an electron and a positron and they separate off to form
positronium,
J. Phys. B 31, L679 (1998). This is of interest as the region in which
the light particles are unbound plays an important role in
rearrangement
processes in which protonium, a hydrogen-like atom made up of a proton
and
an antiproton, and positronium are formed.
This led on to scattering calculations. The Kohn variational method was
used to carry out a detailed calculation of the scattering of

by
an
H atom at very low temperatures, J. Phys. B 35, L489 (2002). Much work
remains to be done on this scattering process.
Yimin Liu is a PDRA supported by EPSRC. He is currently working on the
scattering of

by helium (He) at very low
temperatures. This
process
is of interest for two reasons. Firstly, experimentalists on the ATHENA
project are very keen to know if collisions with ultracold He could
be used to cool

to the very low temperatures
required for
trapping.
Secondly, He is likely to be one of the main impurities in the ATHENA

trap. Detailed information about the effect on

of
scattering
by He would make it possible to choose the conditions in the trap so as
to
maximise the lifetime of the

.
The He-

system contains three light
particles, two electrons and
a positron. To carry out very accurate calculations on this system we
need to include Hylleraas-type functions in the basis sets in our
variational calculations. These functions contain the distance between
two of the light particles as a linear factor. To include these
functions,
it has been necessary to devise ways of calculating integrals involving
up
to three distances between light particles, two of them linear factors,
the other to the power -1. Integrals involving one and two such factors
were required for Kohn calculations carried out previously of elastic
scattering of a positron by a hydrogen molecule (H
2), J.
Phys. B 23,
3057
(1990).
A method has been devised to calculate the additional integrals
involving
r
ijr
ik/r
jk, where r
ij is
the distance between particles i and j,
required
in He-

calculations. These are
nine-dimensional integrals. In this
method, integration is carried out analytically over seven dimensions,
using
prolate spheroidal coordinates, so that numerical integration is only
required for the two remaining dimensions.
This has made possible the evaluation of a Born-Oppenheimer potential
for He-

from which elastic scattering
cross sections can be
calculated.
In positron scattering the positron may annihilate with a target
electron
to form two or three gamma rays. The annihilation is brought about by
the electromagnetic interaction and in most scattering processes it
has only a small effect.
In

scattering there is the additional
possibility that the
antiproton
may annihilate when it comes in contact with a nucleus. This process
is brought about by the strong nuclear.interaction and is much more
probable than positron annihilation. Taking it into account is
interesting.
The probability of antiproton annihilation may be sufficiently high
that He
is unsuitable for cooling

. The next stage will be to
calculate cross sections for rearrangement
processes that give rise to, for example, antiprotonic He + positronium
or a hydrogen-like ion made up of a He nucleus and an antiproton +
positronium minus, a bound state of two electrons and a positron. These
will be calculated by evaluating the T-matrix elements corresponding to
these processes, using the Born-Oppenheimer elastic scattering wave
function as an approximation to the exact scattering wave function. It
is
hoped eventually to carry out these evaluations using the Kohn method.
It seems that likely that H
2 would be more suitable for
cooling

, as the nuclei have charge +1 as
opposed to + 2, as in the case
of He, and are not located at the nuclear centre of mass. This makes it
likely that the probability that the antiproton in

will
annihilate
is lower in

H
2 scattering than in

He scattering. Also, H
2
is
the likely to be the other main impurity in the

trap, besides
He.
Thus,

scattering by H
2 is a
very interesting process. The
H
2-

system contains three light
particles, as in the case of
He-

. However, H
2 contains
two nuclei which is a serious
complication. As a first step, we intend to use an adapted quantum
chemistry code to calculate a potential energy surface for H
2-

and use it to calculate cross sections for elastic scattering. We will
also
calculate a cross section for antiproton annihilation. This will give
us
some indication of the suitability of H
2 for cooling

.
We are keeping in contact with Professor Charlton and his group at
Swansea, one of the main groups working on the ATHENA project. We are
interested in any of the problems they experience for which a
theoretical
treatment would be helpful.