Degeneracy and strategies of long baseline and reactor experiments

Abstract

Assuming that the JPARC experiment measures the oscillation probabilities $P({\nu }_{\mu }\to {\nu }_e)$ and $P({\bar{\nu }}_{\mu }\to {\bar{\nu }}_e)$ at $|\Delta m_{31}^2|L/4E=\pi /2$, I discuss what kind of extra experiment (long baseline or reactor) can contribute to determination of ${\theta }_{13}$ and the CP phase $\delta$.

3 pages, 3 sets of figures, uses espcrc2.sty. Talk given at 6th International Workshop on Neutrino Factories and Superbeams (NuFact 04), Osaka, Japan, 26 Jul - 1 Aug 2004

References in corpus (1)

• Systematic limits on sin^2{2theta_{13}} in neutrino oscillation experiments with multi-reactors

Cited by in corpus (2)

• Probing the deviation from maximal mixing of atmospheric neutrinos
• ${\nu }_{\mu }$ disappearance at the SPL, T2K-I, NO$\nu$A and the Neutrino Factory