About the Experiment
EXO is an experiment looking
for
neutrinoless double beta decay in
the 136 isotope of Xenon. The experiment current consists
of two facets:
- EXO-200, a 200-kilogram
prototype experiment currently being installed and
commissioned at WIPP. This will measure the - yet
unobserved - two-neutrino mode of double beta decay of
Xenon 136 and provide a competitive limit on
neutrinoless double beta decay.
- EXO - a ton scale experiment using Xenon 136 to
search for neutrinoless double beta decay. The
collaboration is undergoing extensive R&D to develop
the Xenon detector and a way to "tag" the products of
the decay in order to eliminate all backgrounds.
There are many advantages to using a noble element,
specifically Xenon. It is relatively easy to purify the
LXe, which allows it to be reused in different detectors.
It is relatively easy to enrich to the 136 isotope using
Russian centrifuges. The Xenon 136 Q-value - the energy
of the decay - is 2.48 MeV, which is high enough to be
above many of the Uranium lines. In using LXe as a
scintillator in our detector we avoid needing additional
materials and we are able to achieve great energy
resolution through collecting both ionization electrons
and scintillation light. Finally, using Xenon
allows for complete background elimination through tagging
of the daughter Barium ion.
Neutrinoless Double Beta Decay
Neutrinoless double beta decay is a special case of beta
decay. Beta decay is a common form of nuclear decay which
occurs when a neutron in an unstable nucleus emits an
electron and an antineutrino and becomes a proton. There are
version of it where positrons or neutrinos are absorbed,
or a proton becomes a neutron.
Double beta decay occurs when a nucleus is energetically
forbidden to decay through single beta decay. While it
has been predicted to exist for a long time, double beta
decay was first observed in 1986. Many isotopes are
theorized to undergo double beta decay, including Xenon
136. In normal double beta decay, two electrons and two
antineutrinos are ejected from the nucleus when two
neutrons become protons. The half-lives of double beta
decay isotopes are very long, about 10^20 years. This is
more than a billion times longer than the age of the
universe! So if you started with 8 billion atoms that can
undergo double beta decay at the beginning of the
universe, you would expect about 1 to have decayed by now.
Neutrinoless double beta decay has not yet been seen, but
is predicted to exist. It is like normal double beta
decay, but because of special roperties of the neutrino,
no neutrinos would be emitted from the nucleus. In order
for this to occur, the neutrino must be its own
antiparticle. Since the discovery that neutrinoes have a
(very small) mass, it is thought that they are Majorona
particles, which means they are their own antiparticle.
Many particles have an antiparticle partner - the electron
has the positron, for instance. The neutral pion is its own antiparticle.
We want to see neutrinoless double beta decay for two reasons. First,
we don't know if the neutrino is its own antiparticle or not, and
seeing it would answer this question for sure. Second, we don't know
the exact mass of the neutrino and a measurement of the neutrinoless
double beta decay half life would allow us to measure the neutrino
mass. Even if we don't see neutrinoless double beta decay, a limit on
the half life places a limit on the neutrino mass. EX0-200 may not
see neutrinoless double beta decay, but it should be able to improve
the limit on the half life.
EXO-200
EXO-200 is a prototype to develop techniques of working with liquid
xenon in a time projection chamber (TPC). One possibility
for ton-scale EXO is a liquid TPC, so familiarity with
EXO-200 technologies will contribute to the design of
ton-scale EXO. Additionally, EXO-200 provides a testing
ground for developing and procuring extremely radiopure
materials and removing backgrounds. EXO-200 will provide
fundamental competitive science measurements, such as a
measurement of the (not yet observed) double beta decay of
Xenon 136 and an improved limit
on
neutrinoless double beta decay.
We are using 200 kg of liquid Xenon (LXe) enriched to 80% of the 136 isotope
for EXO-200. The LXe fills our TPC vessel. When an event
occurs the energetic electrons interacts with the LXe to
create scintillation light that we detect with Avalanche
Photodiodes (APD's). The energetic electrons also ionize
some of the Xenon and the ionized electrons drift to
charge collection wires at the ends of the vessel in an
electric field. The time between the light pulse and the
electrons reaching the wires tell us how far in the event
occurred since we know the drift time.
The TPC vessel is contained within a cryostat system to help keep the
Xenon at liquid temperature. The vessel is contained in a volume of
HFE, a cryogenic buffer fluid. The HFE is within a large copper
cryostat, which is then inside another coper cryostat with a vacuum
gap in between. The cryostat is shielded with lead and contained in a
class-100 cleanroom. This helps prevent radioactive backgrounds. All
materials contained within the lead have been extensively counted for
radiopurity. Materials have been chosen to be low in radioactive
isotopes and contamination. The majority of the material is ultrapure
copper, teflon, phosphorbronze, and acrylic.