Working with antimatter presents several experimental challenges. Magnetic traps—wherein neutral atoms are trapped using their
magnetic moments—are required to keep antimatter from annihilating with matter, but are notoriously weak. Only atoms with kinetic energies equivalent to less than one kelvin may be trapped. The
ATHENA and
ATRAP (AD-2) projects produced antihydrogen by merging cold
plasmas of
positrons and
antiprotons. While this method has been quite successful, it creates antimatter atoms with kinetic energies too large to be trapped. Moreover, to do
laser spectroscopy on these antimatter atoms, they need to be in their
ground state, something that does not appear to be the case for the majority of antimatter atoms created with this technique. Antiprotons are received from the antiproton decelerator and are 'mixed' with positrons from a specially designed positron accumulator in a versatile
Penning trap. The central region where the mixing and thus antihydrogen formation takes place is surrounded by a
superconducting octupole magnet and two axially separated short solenoid "mirror-coils" to form a "minimum-
B" magnetic trap. Once trapped, antihydrogen can be subjected to study, and the measurements compared to those of hydrogen.
Antihydrogen detection In order to detect trapped antihydrogen, ALPHA also includes a 'silicon vertex detector': a cylindrical detector composed of three layers of silicon strips. Each strip acts as a detector for the charged particles passing through. By recording how the strips are excited, ALPHA can reconstruct the traces of particles traveling through the detector. When an antiproton annihilates, the process typically results in the emission of 3 or 4 charged
pions. By reconstructing their traces through the detector, the location of the annihilation can be determined. These traces are quite distinct from those of
cosmic rays also detected, but due to their high energy they pass straight through the detector. To confirm successful trapping, the ALPHA magnet that creates the minimum B-field was designed to allow rapid and repeated de-energizing. The decay of current during de-energization has a characteristic duration of 9 ms, orders of magnitude faster than similar systems. In theory, the fast turn-off speed and the ability to suppress false cosmic rays signals allows ALPHA to detect the release of single antihydrogen atoms during de-energization.
Cooling antihydrogen One of the main challenges of working with antihydrogen is cooling it enough to be able to trap it. Antiprotons and positrons are not easily cooled to
cryogenic temperatures, so in order to do this ALPHA has implemented a well known technique from atomic physics known as
evaporative cooling. State-of-the art minimum-B traps such as the one ALPHA uses have depths of order 1 Kelvin. == Results ==