Abstract
The T2K experiment presents new measurements of neutrino oscillation parameters using
$$19.7(16.3)\times 10^{20}$$
19.7
(
16.3
)
×
10
20
protons on target (POT) in (anti-)neutrino mode at ...the far detector (FD). Compared to the previous analysis, an additional
$$4.7\times 10^{20}$$
4.7
×
10
20
POT neutrino data was collected at the FD. Significant improvements were made to the analysis methodology, with the near-detector analysis introducing new selections and using more than double the data. Additionally, this is the first T2K oscillation analysis to use NA61/SHINE data on a replica of the T2K target to tune the neutrino flux model, and the neutrino interaction model was improved to include new nuclear effects and calculations. Frequentist and Bayesian analyses are presented, including results on
$$\sin ^2\theta _{13}$$
sin
2
θ
13
and the impact of priors on the
$$\delta _{\textrm{CP}}$$
δ
CP
measurement. Both analyses prefer the normal mass ordering and upper octant of
$$\sin ^2\theta _{23}$$
sin
2
θ
23
with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on
$$\sin ^2\theta _{13}$$
sin
2
θ
13
from reactors,
$$\sin ^2\theta _{23}=0.561^{+0.021}_{-0.032}$$
sin
2
θ
23
=
0
.
561
-
0.032
+
0.021
using Feldman–Cousins corrected intervals, and
$$\varDelta {}m^2_{32}=2.494_{-0.058}^{+0.041}\times 10^{-3}~\text {eV}^2$$
Δ
m
32
2
=
2
.
494
-
0.058
+
0.041
×
10
-
3
eV
2
using constant
$$\varDelta \chi ^{2}$$
Δ
χ
2
intervals. The CP-violating phase is constrained to
$$\delta _{\textrm{CP}}=-1.97_{-0.70}^{+0.97}$$
δ
CP
=
-
1
.
97
-
0.70
+
0.97
using Feldman–Cousins corrected intervals, and
$$\delta _{\textrm{CP}}=0,\pi $$
δ
CP
=
0
,
π
is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than
$$2\sigma $$
2
σ
credible level using a flat prior in
$$\delta _{\textrm{CP}},$$
δ
CP
,
and just below
$$2\sigma $$
2
σ
using a flat prior in
$$\sin \delta _{\textrm{CP}}.$$
sin
δ
CP
.
When the external constraint on
$$\sin ^2\theta _{13}$$
sin
2
θ
13
is removed,
$$\sin ^2\theta _{13}=28.0^{+2.8}_{-6.5}\times 10^{-3},$$
sin
2
θ
13
=
28
.
0
-
6.5
+
2.8
×
10
-
3
,
in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.
The T2K experiment presents new measurements of neutrino oscillation parameters using
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\begin{document}$$19.7(16.3)\times 10^{20}$$\end{document}
19.7
(
16.3
)
×
10
20
protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional
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\begin{document}$$4.7\times 10^{20}$$\end{document}
4.7
×
10
20
POT neutrino data was collected at the FD. Significant improvements were made to the analysis methodology, with the near-detector analysis introducing new selections and using more than double the data. Additionally, this is the first T2K oscillation analysis to use NA61/SHINE data on a replica of the T2K target to tune the neutrino flux model, and the neutrino interaction model was improved to include new nuclear effects and calculations. Frequentist and Bayesian analyses are presented, including results on
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\begin{document}$$\sin ^2\theta _{13}$$\end{document}
sin
2
θ
13
and the impact of priors on the
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\begin{document}$$\delta _{\textrm{CP}}$$\end{document}
δ
CP
measurement. Both analyses prefer the normal mass ordering and upper octant of
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\begin{document}$$\sin ^2\theta _{23}$$\end{document}
sin
2
θ
23
with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on
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\begin{document}$$\sin ^2\theta _{13}$$\end{document}
sin
2
θ
13
from reactors,
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\begin{document}$$\sin ^2\theta _{23}=0.561^{+0.021}_{-0.032}$$\end{document}
sin
2
θ
23
=
0
.
561
-
0.032
+
0.021
using Feldman–Cousins corrected intervals, and
\documentclass12pt{minimal}
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\begin{document}$$\varDelta {}m^2_{32}=2.494_{-0.058}^{+0.041}\times 10^{-3}~\text {eV}^2$$\end{document}
Δ
m
32
2
=
2
.
494
-
0.058
+
0.041
×
10
-
3
eV
2
using constant
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\setlength{\oddsidemargin}{-69pt}
\begin{document}$$\varDelta \chi ^{2}$$\end{document}
Δ
χ
2
intervals. The CP-violating phase is constrained to
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\begin{document}$$\delta _{\textrm{CP}}=-1.97_{-0.70}^{+0.97}$$\end{document}
δ
CP
=
-
1
.
97
-
0.70
+
0.97
using Feldman–Cousins corrected intervals, and
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\begin{document}$$\delta _{\textrm{CP}}=0,\pi $$\end{document}
δ
CP
=
0
,
π
is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than
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\begin{document}$$2\sigma $$\end{document}
2
σ
credible level using a flat prior in
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\begin{document}$$\delta _{\textrm{CP}},$$\end{document}
δ
CP
,
and just below
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\begin{document}$$2\sigma $$\end{document}
2
σ
using a flat prior in
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\begin{document}$$\sin \delta _{\textrm{CP}}.$$\end{document}
sin
δ
CP
.
When the external constraint on
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\begin{document}$$\sin ^2\theta _{13}$$\end{document}
sin
2
θ
13
is removed,
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\begin{document}$$\sin ^2\theta _{13}=28.0^{+2.8}_{-6.5}\times 10^{-3},$$\end{document}
sin
2
θ
13
=
28
.
0
-
6.5
+
2.8
×
10
-
3
,
in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.
Abstract The T2K experiment presents new measurements of neutrino oscillation parameters using $$19.7(16.3)\times 10^{20}$$ 19.7 ( 16.3 ) × 10 20 protons on target (POT) in (anti-)neutrino mode at ...the far detector (FD). Compared to the previous analysis, an additional $$4.7\times 10^{20}$$ 4.7 × 10 20 POT neutrino data was collected at the FD. Significant improvements were made to the analysis methodology, with the near-detector analysis introducing new selections and using more than double the data. Additionally, this is the first T2K oscillation analysis to use NA61/SHINE data on a replica of the T2K target to tune the neutrino flux model, and the neutrino interaction model was improved to include new nuclear effects and calculations. Frequentist and Bayesian analyses are presented, including results on $$\sin ^2\theta _{13}$$ sin 2 θ 13 and the impact of priors on the $$\delta _{\textrm{CP}}$$ δ CP measurement. Both analyses prefer the normal mass ordering and upper octant of $$\sin ^2\theta _{23}$$ sin 2 θ 23 with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on $$\sin ^2\theta _{13}$$ sin 2 θ 13 from reactors, $$\sin ^2\theta _{23}=0.561^{+0.021}_{-0.032}$$ sin 2 θ 23 = 0 . 561 - 0.032 + 0.021 using Feldman–Cousins corrected intervals, and $$\varDelta {}m^2_{32}=2.494_{-0.058}^{+0.041}\times 10^{-3}~\text {eV}^2$$ Δ m 32 2 = 2 . 494 - 0.058 + 0.041 × 10 - 3 eV 2 using constant $$\varDelta \chi ^{2}$$ Δ χ 2 intervals. The CP-violating phase is constrained to $$\delta _{\textrm{CP}}=-1.97_{-0.70}^{+0.97}$$ δ CP = - 1 . 97 - 0.70 + 0.97 using Feldman–Cousins corrected intervals, and $$\delta _{\textrm{CP}}=0,\pi $$ δ CP = 0 , π is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than $$2\sigma $$ 2 σ credible level using a flat prior in $$\delta _{\textrm{CP}},$$ δ CP , and just below $$2\sigma $$ 2 σ using a flat prior in $$\sin \delta _{\textrm{CP}}.$$ sin δ CP . When the external constraint on $$\sin ^2\theta _{13}$$ sin 2 θ 13 is removed, $$\sin ^2\theta _{13}=28.0^{+2.8}_{-6.5}\times 10^{-3},$$ sin 2 θ 13 = 28 . 0 - 6.5 + 2.8 × 10 - 3 , in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.
This paper presents the first combined measurement of the double-differential muon neutrino and antineutrino charged-current cross sections with no pions in the final state on hydrocarbon at the ...off-axis near detector of the T2K experiment. The data analyzed in this work comprise 5.8\(\times\)10\(^{20}\) and 6.3\(\times\)10\(^{20}\) protons on target in neutrino and antineutrino mode respectively, at a beam energy peak of 0.6 GeV. Using the two measured cross sections, the sum, difference and asymmetry were calculated with the aim of better understanding the nuclear effects involved in such interactions. The extracted measurements have been compared with the prediction from different Monte Carlo generators and theoretical models showing that the difference between the two cross sections have interesting sensitivity to nuclear effects.
This paper reports the first simultaneous measurement of the double differential muon neutrino charged-current cross section on oxygen and carbon without pions in the final state as a function of the ...outgoing muon kinematics, made at the ND280 off-axis near detector of the T2K experiment. The ratio of the oxygen and carbon cross sections is also provided to help validate various models' ability to extrapolate between carbon and oxygen nuclear targets, as is required in T2K oscillation analyses. The data are taken using a neutrino beam with an energy spectrum peaked at 0.6 GeV. The extracted measurement is compared with the prediction from different Monte Carlo neutrino-nucleus interaction event generators, showing particular model separation for very forward-going muons. Overall, of the models tested, the result is best described using Local Fermi Gas descriptions of the nuclear ground state with RPA suppression.
The electron (anti-)neutrino component of the T2K neutrino beam constitutes the largest background in the measurement of electron (anti-)neutrino appearance at the far detector. The electron neutrino ...scattering is measured directly with the T2K off-axis near detector, ND280. The selection of the electron (anti-)neutrino events in the plastic scintillator target from both neutrino and anti-neutrino mode beams is discussed in this paper. The flux integrated single differential charged-current inclusive electron (anti-)neutrino cross-sections, \(d\sigma/dp\) and \(d\sigma/d\cos(\theta)\), and the total cross-sections in a limited phase-space in momentum and scattering angle (\(p > 300\) MeV/c and \(\theta \leq 45^{\circ}\)) are measured using a binned maximum likelihood fit and compared to the neutrino Monte Carlo generator predictions, resulting in good agreement.
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