Abstract

This work extends the idea of using a cyclotron-based antineutrino source for purposes of neutrino physics. Long baseline experiments suffer from degeneracies and correlations between , and the mass hierarchy. However, the combination of a superconducting cyclotron and a big liquid scintillator detector like JUNO in a medium baseline experiment, which does not depend on the mass hierarchy, may allow to determine whether the position of the mixing angle is in the lower octant or the upper octant. Such an experiment would improve the precision of the measurement to a degree which depends on the CP-phase.

Highlights

  • The yellow area shows the 68.3% confidence interval, within which the experiment is insensitive to octant degeneracy

  • For these values a 5 MW cyclotron can distinguish the octant, if the mixing angle Θ23 is outside the range 38.5o − 52.9o

  • Increasing statistics causes an improvement in the sensitivity

Read more

Summary

Proposal of the experimental setup

The full description of our proposal is presented in [6], which is based on the DAEδALUS experiment project [7]. Where ∆ij = ∆m2ij ·L/(4Eν); ∆m2ij – the neutrino mass squared difference; L – the distance between source and detector; Eν – neutrino energy; δCP – Dirac phase of CP violation. Two cyclotrons (near and far) will be located at distances 1.5 km and 20 km respectively. The power of the near cyclotron is 1 MW. NH is assumed, because at the distance 20 km the experiment is insensitive to mass hierarchy. It is clear, that neutrino rate increases with the mixing angle Θ23

Statistical evaluation of MC simulations
Sensitivity to discovery of true octant
The accuracy of Θ23 measurement
Monte-Carlo simulations
Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call