Daya Bay Measures the Neutrino Mixing Parameter sin22θ13
In a letter submitted to the Physical Review (
arXiv:1203.1669[hep-ex]),
the Daya Bay Collaboration, including members of Virginia Tech's Center for Neutrino Physics, announces the first
observation and measurement on the neutrino mixing parameter sin
22θ
13. The mixing
angle θ
13 governs the rate of electron neutrino conversion to muon and tau neutrinos at baselines
consistent with atmospheric oscillations. The hunt for theta;
13 is currently the focus of several
major experiments world wide, who are using either electron antineutrinos from nuclear reactors or beams of muon
neutrios/anitneutrinos produced at accelerators.
In reactor neutrino experiments such as Daya Bay, the oscillation is observed as an electron
antineutrino disappearance at a distance of about 2 km from the reactor. The effect can only be measured
with confidence in the comparison of detectors placed near the reactor cores which measure the neutrino flux
before significant oscillation has occured to detectors placed farther away at a location close to
the oscillation maximum. In this way uncertainties associated with antineutrino production in the reactor, the
interaction cross section in the detector, and to a lessor degree detector efficiency will cancel in the near/far
detector comparison. Daya Bay Collaboration is the first to apply this technique and report results, finding
sin22θ13 = 0.092±0.016(stat.)±0.005(syst.).
Read the full press release

The measured vs. expected signal in each detector, assuming no oscillation. Reactor and survey data are used to
compute the weighted average baselines. The oscillation survival probability at the best fit value is given by
the smooth curve.

The far detector hall showing three antineurino detectors in the water pool as it is being filled. The far hall
is where a deficit of reactor antineutinos was observed relative to the near detector sites. This is the signature
of neutrino oscillations and the basis of the discovery and measurement of the oscillation parameter
sin
22θ
13.
(Photo by Joseph Hor © Virginia Tech)
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