| Most of our current knowledge of the Universe comes from the
observation of photons.
Photons have many advantages as cosmic
information carriers: they are copiously produced, they are stable and
electrically neutral, they are easy to detect over a wide energy range,
and their spectrum carries detailed information about the chemical and
physical properties of the source.
Their disadvantage is that the hot,
dense regions which form the central engines of stars, active galactic
nuclei and other astrophysical energy sources are completely opaque to
photons, and therefore we cannot investigate the properties of these
regions by direct observation, but only by indirect inference. For
example, the photons we observe from the Sun come from its photosphere,
far removed from the hydrogen-fusing core. Moreover, high energy photons
interact with photons of the infrared radiation background and with the
cosmic microwave background to create electron-positron pairs; this is
the Greisen-Zatsepin-Kuz'min effect (GZK).
This effect suppresses any possibility of surveying the sky over
distances greater than 100Mpc with high energy (>10 TeV) gamma rays.
In order to observe the inner workings of the astrophysical objects
and to obtain a description of the Universe over a larger range of
energies, we need a probe which is electrically neutral, so that its
trajectory will not be affected by magnetic fields, stable so that it
will reach us from distant sources, and weakly interacting so that it
will penetrate regions which are opaque to photons. The only candidate
currently known to exist is the neutrino.
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| Some astrophysical sources are known to emit neutrinos: hydrogen
fusion produces electron neutrinos as by-products, and solar neutrino
astronomy has a 30 years long history; the conversion of iron
nuclei to neutrons when a neutron star is formed in the heart of a
supernova produces a burst of neutrinos (augmented by the thermal
production of neutrino-antineutrino pairs), and one such burst was
observed by Kamiokande and IMB for Supernova 1987A; cosmology predicts a
low-energy relic neutrino background similar to the low-energy relic
photons of the Cosmic Microwave Background, but these would have an
effective temperature of around 1.9 K and are very difficult to observe.
Astrophysical sources of high-energy neutrinos have not been observed
directly, but their existence can be inferred from the properties of
cosmic rays.
Primary cosmic rays are protons, with some admixture of
heavier nuclei; the energy spectrum is a power law which extends to
extremely high energies, values exceeding 1020 eV having been
observed in recent years. Protons themselves have limited use as
astrophysical information carriers because they are charged, and
therefore subject to deflection by cosmic magnetic fields: only the very
highest-energy cosmic rays are likely to retain any memory of the source
direction. The exact source of the high-energy cosmic rays is thus
unknown, although supernova remnants and active galactic nuclei have
been proposed. Whatever the source, it is clear that accelerating
protons to such high energies is likely to generate a large associated
flux of photo-produced pions, which decay to yield gamma rays and
neutrinos. These will remember the source direction, and so the
existence of a general flux of very high energy cosmic-ray protons
implies the existence of sources of high-energy neutrinos. Neutrino astronomy thus offers the possibility of observing sources
which correspond to the central engines of the most energetic
astrophysical phenomena. It can also provides long
baselines for neutrino oscillation studies, and can explore useful
regions of supersymmetric parameter space in the context of dark matter.
The drawback, of course, is that the weak interactions of neutrinos
imply that a very massive detector with extremely good background
rejection is required to observe a measurable flux.
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