Abstract

We study the physics potential of the long-baseline experiments T2HK, T2HKK and ESSνSB in the context of invisible neutrino decay. We consider normal mass ordering and assume the state ν3 as unstable, decaying into sterile states during the flight and obtain constraints on the neutrino decay lifetime (τ3). We find that T2HK, T2HKK and ESSνSB are sensitive to the decay-rate of ν3 for τ3/m3 ≤ 2.72 × 10−11s/eV, τ3/m3 ≤ 4.36 × 10−11s/eV and τ3/m3 ≤ 2.43 × 10−11s/eV respectively at 3σ C.L. We compare and contrast the sensitivities of the three experiments and specially investigate the role played by the mixing angle θ23. It is seen that for experiments with flux peak near the second oscillation maxima, the poorer sensitivity to θ23 results in weaker constraints on the decay lifetime. Although, T2HKK has one detector close to the second oscillation maxima, having another detector at the first oscillation maxima results in superior sensitivity to decay. In addition, we find a synergy between the two baselines of the T2HKK experiment which helps in giving a better sensitivity to decay for θ23 in the higher octant. We discuss the octant sensitivity in presence of decay and show that there is an enhancement in sensitivity which occurs due to the contribution from the survival probability Pμμ is more pronounced for the experiments at the second oscillation maxima. We also obtain the combined sensitivity of T2HK+ESSνSB and T2HKK+ESSνSB as τ3/m3 ≤ 4.36 × 10−11s/eV and τ3/m3 ≤ 5.53 × 10−11s/eV respectively at 3σ C.L.

Highlights

  • We study the physics potential of the long-baseline experiments T2HK, T2HKK and ESSνSB in the context of invisible neutrino decay

  • We find that T2HK, T2HKK and ESSνSB are sensitive to the decay-rate of ν3 for τ3/m3 ≤ 2.72 × 10−11s/eV, τ3/m3 ≤ 4.36 × 10−11s/eV and τ3/m3 ≤ 2.43 × 10−11s/eV respectively at 3σ C.L

  • We have examined the physics potential of future long-baseline experiments T2HK/T2HKK and ESSνSB in the context of invisible neutrino decay

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Summary

Neutrino oscillation in presence of invisible decay of neutrino

We discuss the propagation of neutrinos in presence of invisible neutrino decay. We assume that the ν3 is unstable and it decays into a sterile neutrino and a singlet scalar (ν3 → ν4 + J) with lifetime τ3. In this case we can extend the mass and flavour bases by νi ν4 T and να νs T , where i = 1, 2, 3 and α = νe, νμ, ντ. We assume that the decay eigenstates and the mass-eigenstates are same. Under these assumptions, we can write the neutrino evolution in presence of matter in the following way. An experiment is sensitive to the values of α where, α ∼ E/L. Sensitivity is expected to be more at the second oscillation maxima as compared to the first oscillation maxima

Experimental details
ESSνSB
Simulation details
Results
Sensitivity to the decay
Synergy between 295 km and 1100 km baselines
Role of decay in the θ23 determination
Combined analysis
Summary & conclusions
Full Text
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