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ATHENA, also known as the AD-1 experiment, was an
antimatter In modern physics, antimatter is defined as matter composed of the antiparticles (or "partners") of the corresponding particles in "ordinary" matter. Antimatter occurs in natural processes like cosmic ray collisions and some types of radio ...
research project at the
Antiproton Decelerator The Antiproton Decelerator (AD) is a storage ring at the CERN laboratory near Geneva. It was built from the Antiproton Collector (AC) to be a successor to the Low Energy Antiproton Ring (LEAR) and started operation in the year 2000. Antipro ...
at CERN, Geneva. In August 2002, it was the first experiment to produce 50,000 low-energy
antihydrogen Antihydrogen () is the antimatter counterpart of hydrogen. Whereas the common hydrogen atom is composed of an electron and proton, the antihydrogen atom is made up of a positron and antiproton. Scientists hope that studying antihydrogen may shed ...
atoms, as reported in ''
Nature Nature, in the broadest sense, is the physical world or universe. "Nature" can refer to the phenomena of the physical world, and also to life in general. The study of nature is a large, if not the only, part of science. Although humans ar ...
''. In 2005, ATHENA was disbanded and many of the former members of the research team worked on the subsequent
ALPHA experiment The Antihydrogen Laser Physics Apparatus (ALPHA), also known as AD-5, is an experiment at the Antiproton Decelerator at CERN, designed to trap neutral antihydrogen in a magnetic trap, and conduct experiments on them. The ultimate goal of this ...
.


Experimental setup

The ATHENA apparatus comprised four main subsystems: the
antiproton The antiproton, , (pronounced ''p-bar'') is the antiparticle of the proton. Antiprotons are stable, but they are typically short-lived, since any collision with a proton will cause both particles to be annihilated in a burst of energy. The exi ...
catching trap, the positron accumulator, the antiproton/positron mixing trap, and the antihydrogen annihilation detector. All traps in the experiment were variations of the
Penning trap A Penning trap is a device for the storage of charged particles using a homogeneous axial magnetic field and an inhomogeneous quadrupole electric field. This kind of trap is particularly well suited to precision measurements of properties of i ...
, which uses an axial
magnetic field A magnetic field is a vector field that describes the magnetic influence on moving electric charges, electric currents, and magnetic materials. A moving charge in a magnetic field experiences a force perpendicular to its own velocity and t ...
to transversely confine the charged particles, and a series of hollow cylindrical electrodes to trap them axially. The catching and mixing traps were adjacent to each other, and coaxial with a 3 T magnetic field from a
superconducting Superconductivity is a set of physical properties observed in certain materials where electrical resistance vanishes and magnetic flux fields are expelled from the material. Any material exhibiting these properties is a superconductor. Unlike ...
solenoid upright=1.20, An illustration of a solenoid upright=1.20, Magnetic field created by a seven-loop solenoid (cross-sectional view) described using field lines A solenoid () is a type of electromagnet formed by a helix, helical coil of wire whose ...
. The positron accumulator had its own magnetic system, also a solenoid, with a field strength of 0.14
Tesla Tesla most commonly refers to: * Nikola Tesla (1856–1943), a Serbian-American electrical engineer and inventor * Tesla, Inc., an American electric vehicle and clean energy company, formerly Tesla Motors, Inc. * Tesla (unit) (symbol: T), the SI-d ...
. A separate
cryogenic In physics, cryogenics is the production and behaviour of materials at very low temperatures. The 13th IIR International Congress of Refrigeration (held in Washington DC in 1971) endorsed a universal definition of “cryogenics” and “cr ...
heat exchanger in the bore of the superconducting magnet cooled the catching and mixing traps to about 15 K. The ATHENA apparatus featured an open, modular design that allowed experimental flexibility, particularly in introducing large numbers of
positrons The positron or antielectron is the antiparticle or the antimatter counterpart of the electron. It has an electric charge of +1 '' e'', a spin of 1/2 (the same as the electron), and the same mass as an electron. When a positron collides ...
into the apparatus.


Catching trap

The catching trap slowed, trapped, cooled, and accumulated
antiprotons The antiproton, , (pronounced ''p-bar'') is the antiparticle of the proton. Antiprotons are stable, but they are typically short-lived, since any collision with a proton will cause both particles to be annihilated in a burst of energy. The exi ...
. To cool antiprotons, the catching trap was first loaded with electrons, which cooled by synchrotron radiation in the 3 Tesla magnetic field. Typically, the AD delivered antiprotons having kinetic energy 5.3 MeV and a pulse duration of 200 ns to the experiment at 100 s intervals. The antiprotons were slowed in a thin foil and trapped using a pulsed electric field. The antiprotons lost energy and equilibrated with the cold electrons by
Coulomb interaction Coulomb's inverse-square law, or simply Coulomb's law, is an experimental law of physics that quantifies the amount of force between two stationary, electrically charged particles. The electric force between charged bodies at rest is conventio ...
. The electrons were ejected before mixing the antiprotons with positrons. Each AD shot resulted in about cold antiprotons for interaction experiments.


Positron accumulator

The positron accumulator slowed, trapped and accumulated positrons emitted from a radioactive source (1. Bq 22Na). Accumulation for 300 s yields 1. positrons, 50% of which were transferred to the mixing trap, where they cooled by synchrotron radiation.


Mixing trap

The mixing trap had the axial potential configuration of a nested Penning trap, which permitted two plasmas of opposite charge to come into contact. In ATHENA, the spheroidal positron cloud could be characterized by exciting and detecting axial plasma oscillations. Typical conditions were: stored positrons, a radius of 2 – 2.5 mm, a length of 32 mm, and a maximum density of 2.. An
antihydrogen Antihydrogen () is the antimatter counterpart of hydrogen. Whereas the common hydrogen atom is composed of an electron and proton, the antihydrogen atom is made up of a positron and antiproton. Scientists hope that studying antihydrogen may shed ...
annihilation detector was situated coaxially with the mixing region, between the trap outer radius and the magnet bore.


Antihydrogen annihilation detector

The detector was designed to provide unambiguous evidence for antihydrogen production by detecting the temporally and spatially coincident
annihilation In particle physics, annihilation is the process that occurs when a subatomic particle collides with its respective antiparticle to produce other particles, such as an electron colliding with a positron to produce two photons. The total energy ...
s of the antiproton and positron when a neutral antihydrogen atom escaped the electromagnetic trap and struck the trap electrodes. An antiproton typically annihilates into a few charged or neutral pions. The charged pions were detected by two layers of double-sided, position sensitive, silicon microstrips. The path of a charged particle passing through both layers could be reconstructed, and two or more intersecting tracks allowed determination of the position, or vertex, of the antiproton annihilation. The uncertainty in vertex determination was approximately 4 mm and is dominated by the unmeasured curvature of the charged
pion In particle physics, a pion (or a pi meson, denoted with the Greek letter pi: ) is any of three subatomic particles: , , and . Each pion consists of a quark and an antiquark and is therefore a meson. Pions are the lightest mesons and, more gen ...
s' trajectories in the magnetic field. The temporal coincidence window was approximately 5 microseconds. The solid angle coverage of the interaction region was about 80% of 4π. A positron annihilating with an electron yields two or three photons. The positron detector, comprising 16 rows each containing 12 scintillating, pure cesium-iodide-crystals, was designed to detect the two-photon events, consisting of two 511 keV photons which are always emitted back-to-back. The energy resolution of the detector was 18% full width half maximum at 511 keV, and the photo-peak detection efficiency for single photons was about 20%. The maximum readout rate of the whole detector was about 40 Hz. Ancillary detectors included large scintillator paddles external to the magnet, and a thin, position sensitive, silicon diode through which the incident antiproton beam passed before entering the catching trap. To produce antihydrogen atoms, a positron well in the mixing region was filled with about positrons and allowed to cool to the ambient temperature (15 degrees Kelvin). The nested trap was then formed around the positron well. Next, approximately 104 antiprotons were launched into the mixing region by pulsing the trap from one potential configuration to another. The mixing time is 190 s, after which all particles were dumped and the process repeated. Events triggering the imaging silicon detector (three sides hit in the outer layer) initiated readout of both the silicon and the CsI modules. Using this method, ATHENA could produce – for the first time – several thousands of cold antihydrogen atoms in 2002.


ATHENA collaboration

The ATHENA collaboration comprised the following institutions:


References

{{Reflist


External links

* Record fo
ATHENA
experiment on
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