Measurements of neutrino oscillation parameters from the T2K experiment using 3.6 x 1021 protons on target

Publication type:
Journal article
Metadata:
Autoren
  • K Abe
  • N Akhlaq
  • R Akutsu
  • A Ali
  • S Alonso Monsalve
  • C Alt
  • C Andreopoulos
  • M Antonova
  • S Aoki
  • T Arihara
  • Y Asada
  • Y Ashida
  • ET Atkin
  • M Barbi
  • GJ Barker
  • G Barr
  • D Barrow
  • M Batkiewicz-Kwasniak
  • F Bench
  • V Berardi
  • L Berns
  • S Bhadra
  • A Blanchet
  • A Blondel
  • S Bolognesi
  • T Bonus
  • S Bordoni
  • SB Boyd
  • A Bravar
  • C Bronner
  • S Bron
  • A Bubak
  • M Buizza Avanzini
  • JA Caballero
  • NF Calabria
  • S Cao
  • D Carabadjac
  • AJ Carter
  • SL Cartwright
  • MG Catanesi
  • A Cervera
  • J Chakrani
  • D Cherdack
  • PS Chong
  • G Christodoulou
  • A Chvirova
  • M Cicerchia
  • J Coleman
  • G Collazuol
  • L Cook
  • A Cudd
  • C Dalmazzone
  • T Daret
  • Yu I Davydov
  • A De Roeck
  • G De Rosa
  • T Dealtry
  • CC Delogu
  • C Densham
  • A Dergacheva
  • F Di Lodovico
  • S Dolan
  • D Douqa
  • TA Doyle
  • O Drapier
  • J Dumarchez
  • P Dunne
  • K Dygnarowicz
  • A Eguchi
  • S Emery-Schrenk
  • G Erofeev
  • A Ershova
  • G Eurin
  • D Fedorova
  • S Fedotov
  • M Feltre
  • AJ Finch
  • GA Fiorentini Aguirre
  • G Fiorillo
  • MD Fitton
  • JM Franco Patino
  • M Friend
  • Y Fujii
  • Y Fukuda
  • K Fusshoeller
  • L Giannessi
  • C Giganti
  • V Glagolev
  • M Gonin
  • J Gonzalez Rosa
  • EAG Goodman
  • A Gorin
  • M Grassi
  • M Guigue
  • DR Hadley
  • JT Haigh
  • P Hamacher-Baumann
  • DA Harris
  • M Hartz
  • T Hasegawa
  • S Hassani
  • NC Hastings
  • Y Hayato
  • D Henaff
  • A Hiramoto
  • M Hogan
  • J Holeczek
  • A Holin
  • T Holvey
  • NT Hong Van
  • T Honjo
  • F Iacob
  • AK Ichikawa
  • M Ikeda
  • T Ishida
  • M Ishitsuka
  • HT Israel
  • K Iwamoto
  • A Izmaylov
  • N Izumi
  • M Jakkapu
  • B Jamieson
  • SJ Jenkins
  • C Jesus-Valls
  • JJ Jiang
  • P Jonsson
  • S Joshi
  • CK Jung
  • PB Jurj
  • M Kabirnezhad
  • AC Kaboth
  • T Kajita
  • H Kakuno
  • J Kameda
  • SP Kasetti
  • Y Kataoka
  • Y Katayama
  • T Katori
  • M Kawaue
  • E Kearns
  • M Khabibullin
  • A Khotjantsev
  • T Kikawa
  • H Kikutani
  • S King
  • V Kiseeva
  • J Kisiel
  • T Kobata
  • H Kobayashi
  • T Kobayashi
  • L Koch
  • S Kodama
  • A Konaka
  • LL Kormos
  • Y Koshio
  • A Kostin
  • T Koto
  • K Kowalik
  • Y Kudenko
  • Y Kudo
  • S Kuribayashi
  • R Kurjata
  • T Kutter
  • M Kuze
  • M La Commara
  • L Labarga
  • K Lachner
  • J Lagoda
  • SM Lakshmi
  • M Lamers James
  • M Lamoureux
  • A Langella
  • J-F Laporte
  • D Last
  • N Latham
  • M Laveder
  • L Lavitola
  • M Lawe
  • Y Lee
  • C Lin
  • S-K Lin
  • RP Litchfield
  • SL Liu
  • W Li
  • A Longhin
  • KR Long
  • A Lopez Moreno
  • L Ludovici
  • X Lu
  • T Lux
  • LN Machado
  • L Magaletti
  • K Mahn
  • M Malek
  • M Mandal
  • S Manly
  • AD Marino
  • L Marti-Magro
  • DGR Martin
  • M Martini
  • JF Martin
  • T Maruyama
  • T Matsubara
  • V Matveev
  • C Mauger
  • K Mavrokoridis
  • E Mazzucato
  • N McCauley
  • J McElwee
  • KS McFarland
  • C McGrew
  • J McKean
  • A Mefodiev
  • GD Megias
  • P Mehta
  • L Mellet
  • C Metelko
  • M Mezzetto
  • E Miller
  • A Minamino
  • O Mineev
  • S Mine
  • M Miura
  • L Molina Bueno
  • S Moriyama
  • S Moriyama
  • P Morrison
  • Th A Mueller
  • D Munford
  • L Munteanu
  • K Nagai
  • Y Nagai
  • T Nakadaira
  • K Nakagiri
  • M Nakahata
  • Y Nakajima
  • A Nakamura
  • H Nakamura
  • K Nakamura
  • KD Nakamura
  • Y Nakano
  • S Nakayama
  • T Nakaya
  • K Nakayoshi
  • CER Naseby
  • TV Ngoc
  • VQ Nguyen
  • K Niewczas
  • S Nishimori
  • Y Nishimura
  • K Nishizaki
  • T Nosek
  • F Nova
  • P Novella
  • JC Nugent
  • HM O'Keeffe
  • L O'Sullivan
  • T Odagawa
  • T Ogawa
  • R Okada
  • W Okinaga
  • K Okumura
  • T Okusawa
  • N Ospina
  • RA Owen
  • Y Oyama
  • V Palladino
  • V Paolone
  • M Pari
  • J Parlone
  • S Parsa
  • J Pasternak
  • M Pavin
  • D Payne
  • GC Penn
  • D Pershey
  • L Pickering
  • C Pidcott
  • G Pintaudi
  • C Pistillo
  • B Popov
  • K Porwit
  • M Posiadala-Zezula
  • YS Prabhu
  • F Pupilli
  • B Quilain
  • T Radermacher
  • E Radicioni
  • B Radics
  • MA Ramirez
  • PN Ratoff
  • M Reh
  • C Riccio
  • E Rondio
  • S Roth
  • N Roy
  • A Rubbia
  • AC Ruggeri
  • CA Ruggles
  • A Rychter
  • K Sakashita
  • F Sanchez
  • G Santucci
  • CM Schloesser
  • K Scholberg
  • M Scott
  • Y Seiya
  • T Sekiguchi
  • H Sekiya
  • D Sgalaberna
  • A Shaikhiev
  • F Shaker
  • A Shaykina
  • M Shiozawa
  • W Shorrock
  • A Shvartsman
  • N Skrobova
  • K Skwarczynski
  • D Smyczek
  • M Smy
  • JT Sobczyk
  • H Sobel
  • FJP Soler
  • Y Sonoda
  • AJ Speers
  • R Spina
  • IA Suslov
  • S Suvorov
  • A Suzuki
  • SY Suzuki
  • Y Suzuki
  • AA Sztuc
  • M Tada
  • S Tairafune
  • S Takayasu
  • A Takeda
  • Y Takeuchi
  • K Takifuji
  • HK Tanaka
  • Y Tanihara
  • M Tani
  • A Teklu
  • VV Tereshchenko
  • N Teshima
  • N Thamm
  • LF Thompson
  • W Toki
  • C Touramanis
  • T Towstego
  • KM Tsui
  • T Tsukamoto
  • M Tzanov
  • Y Uchida
  • M Vagins
  • D Vargas
  • M Varghese
  • G Vasseur
  • C Vilela
  • E Villa
  • WGS Vinning
  • U Virginet
  • T Vladisavljevic
  • T Wachala
  • JG Walsh
  • Y Wang
  • L Wan
  • D Wark
  • MO Wascko
  • A Weber
  • R Wendell
  • MJ Wilking
  • C Wilkinson
  • JR Wilson
  • K Wood
  • C Wret
  • J Xia
  • Y-H Xu
  • K Yamamoto
  • T Yamamoto
  • C Yanagisawa
  • G Yang
  • T Yano
  • K Yasutome
  • N Yershov
  • U Yevarouskaya
  • M Yokoyama
  • Y Yoshimoto
  • N Yoshimura
  • M Yu
  • R Zaki
  • A Zalewska
  • J Zalipska
  • K Zaremba
  • G Zarnecki
  • X Zhao
  • T Zhu
  • M Ziembicki
  • ED Zimmerman
  • M Zito
  • S Zsoldos
Autoren-URL
https://www.webofscience.com/api/gateway?GWVersion=2&SrcApp=fis-test-1&SrcAuth=WosAPI&KeyUT=WOS:001065963300007&DestLinkType=FullRecord&DestApp=WOS_CPL
DOI
10.1140/epjc/s10052-023-11819-x
eISSN
1434-6052
Externe Identifier
  • Clarivate Analytics Document Solution ID: R7FB7
  • PubMed Identifier: 37680254
ISSN
1434-6044
Ausgabe der Veröffentlichung
9
Zeitschrift
EUROPEAN PHYSICAL JOURNAL C
Artikelnummer
ARTN 782
Datum der Veröffentlichung
2023
Status
Published
Titel
Measurements of neutrino oscillation parameters from the T2K experiment using 3.6 x 10<SUP>21</SUP> protons on target
Sub types
  • Article
Ausgabe der Zeitschrift
83

Data source: Web of Science (Lite)

Other metadata sources:
Abstract
<jats:title>Abstract</jats:title><jats:p>The T2K experiment presents new measurements of neutrino oscillation parameters using <jats:inline-formula><jats:alternatives><jats:tex-math>$$19.7(16.3)\times 10^{20}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>19.7</mml:mn> <mml:mrow> <mml:mo>(</mml:mo> <mml:mn>16.3</mml:mn> <mml:mo>)</mml:mo> </mml:mrow> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mn>20</mml:mn> </mml:msup> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional <jats:inline-formula><jats:alternatives><jats:tex-math>$$4.7\times 10^{20}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>4.7</mml:mn> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mn>20</mml:mn> </mml:msup> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> 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 <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin ^2\theta _{13}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mo>sin</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:msub> <mml:mi>θ</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> and the impact of priors on the <jats:inline-formula><jats:alternatives><jats:tex-math>$$\delta _{\textrm{CP}}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>δ</mml:mi> <mml:mtext>CP</mml:mtext> </mml:msub> </mml:math></jats:alternatives></jats:inline-formula> measurement. Both analyses prefer the normal mass ordering and upper octant of <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin ^2\theta _{23}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mo>sin</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:msub> <mml:mi>θ</mml:mi> <mml:mn>23</mml:mn> </mml:msub> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin ^2\theta _{13}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mo>sin</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:msub> <mml:mi>θ</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> from reactors, <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin ^2\theta _{23}=0.561^{+0.021}_{-0.032}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mo>sin</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:msub> <mml:mi>θ</mml:mi> <mml:mn>23</mml:mn> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>0</mml:mn> <mml:mo>.</mml:mo> <mml:msubsup> <mml:mn>561</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>0.032</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.021</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> using Feldman–Cousins corrected intervals, and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\varDelta {}m^2_{32}=2.494_{-0.058}^{+0.041}\times 10^{-3}~\text {eV}^2$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>Δ</mml:mi> <mml:mrow /> <mml:msubsup> <mml:mi>m</mml:mi> <mml:mn>32</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> <mml:mo>.</mml:mo> <mml:msubsup> <mml:mn>494</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>0.058</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.041</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:msup> <mml:mspace /> <mml:msup> <mml:mtext>eV</mml:mtext> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> using constant <jats:inline-formula><jats:alternatives><jats:tex-math>$$\varDelta \chi ^{2}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>Δ</mml:mi> <mml:msup> <mml:mi>χ</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> intervals. The CP-violating phase is constrained to <jats:inline-formula><jats:alternatives><jats:tex-math>$$\delta _{\textrm{CP}}=-1.97_{-0.70}^{+0.97}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>δ</mml:mi> <mml:mtext>CP</mml:mtext> </mml:msub> <mml:mo>=</mml:mo> <mml:mo>-</mml:mo> <mml:mn>1</mml:mn> <mml:mo>.</mml:mo> <mml:msubsup> <mml:mn>97</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>0.70</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.97</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> using Feldman–Cousins corrected intervals, and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\delta _{\textrm{CP}}=0,\pi $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>δ</mml:mi> <mml:mtext>CP</mml:mtext> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>0</mml:mn> <mml:mo>,</mml:mo> <mml:mi>π</mml:mi> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than <jats:inline-formula><jats:alternatives><jats:tex-math>$$2\sigma $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>2</mml:mn> <mml:mi>σ</mml:mi> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> credible level using a flat prior in <jats:inline-formula><jats:alternatives><jats:tex-math>$$\delta _{\textrm{CP}},$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>δ</mml:mi> <mml:mtext>CP</mml:mtext> </mml:msub> <mml:mo>,</mml:mo> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> and just below <jats:inline-formula><jats:alternatives><jats:tex-math>$$2\sigma $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>2</mml:mn> <mml:mi>σ</mml:mi> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> using a flat prior in <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin \delta _{\textrm{CP}}.$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mo>sin</mml:mo> <mml:msub> <mml:mi>δ</mml:mi> <mml:mtext>CP</mml:mtext> </mml:msub> <mml:mo>.</mml:mo> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> When the external constraint on <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin ^2\theta _{13}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mo>sin</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:msub> <mml:mi>θ</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> is removed, <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sin ^2\theta _{13}=28.0^{+2.8}_{-6.5}\times 10^{-3},$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msup> <mml:mo>sin</mml:mo> <mml:mn>2</mml:mn> </mml:msup> <mml:msub> <mml:mi>θ</mml:mi> <mml:mn>13</mml:mn> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>28</mml:mn> <mml:mo>.</mml:mo> <mml:msubsup> <mml:mn>0</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>6.5</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>2.8</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:msup> <mml:mo>,</mml:mo> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.</jats:p>
Autoren
  • K Abe
  • N Akhlaq
  • R Akutsu
  • A Ali
  • S Alonso Monsalve
  • C Alt
  • C Andreopoulos
  • M Antonova
  • S Aoki
  • T Arihara
  • Y Asada
  • Y Ashida
  • ET Atkin
  • M Barbi
  • GJ Barker
  • G Barr
  • D Barrow
  • M Batkiewicz-Kwasniak
  • F Bench
  • V Berardi
  • L Berns
  • S Bhadra
  • A Blanchet
  • A Blondel
  • S Bolognesi
  • T Bonus
  • S Bordoni
  • SB Boyd
  • A Bravar
  • C Bronner
  • S Bron
  • A Bubak
  • M Buizza Avanzini
  • JA Caballero
  • NF Calabria
  • S Cao
  • D Carabadjac
  • AJ Carter
  • SL Cartwright
  • MG Catanesi
  • A Cervera
  • J Chakrani
  • D Cherdack
  • PS Chong
  • G Christodoulou
  • A Chvirova
  • M Cicerchia
  • J Coleman
  • G Collazuol
  • L Cook
  • A Cudd
  • C Dalmazzone
  • T Daret
  • Yu I Davydov
  • A De Roeck
  • G De Rosa
  • T Dealtry
  • CC Delogu
  • C Densham
  • A Dergacheva
  • F Di Lodovico
  • S Dolan
  • D Douqa
  • TA Doyle
  • O Drapier
  • J Dumarchez
  • P Dunne
  • K Dygnarowicz
  • A Eguchi
  • S Emery-Schrenk
  • G Erofeev
  • A Ershova
  • G Eurin
  • D Fedorova
  • S Fedotov
  • M Feltre
  • AJ Finch
  • GA Fiorentini Aguirre
  • G Fiorillo
  • MD Fitton
  • JM Franco Patiño
  • M Friend
  • Y Fujii
  • Y Fukuda
  • K Fusshoeller
  • L Giannessi
  • C Giganti
  • V Glagolev
  • M Gonin
  • J González Rosa
  • EAG Goodman
  • A Gorin
  • M Grassi
  • M Guigue
  • DR Hadley
  • JT Haigh
  • P Hamacher-Baumann
  • DA Harris
  • M Hartz
  • T Hasegawa
  • S Hassani
  • NC Hastings
  • Y Hayato
  • D Henaff
  • A Hiramoto
  • M Hogan
  • J Holeczek
  • A Holin
  • T Holvey
  • NT Hong Van
  • T Honjo
  • F Iacob
  • AK Ichikawa
  • M Ikeda
  • T Ishida
  • M Ishitsuka
  • HT Israel
  • K Iwamoto
  • A Izmaylov
  • N Izumi
  • M Jakkapu
  • B Jamieson
  • SJ Jenkins
  • C Jesús-Valls
  • JJ Jiang
  • P Jonsson
  • S Joshi
  • CK Jung
  • PB Jurj
  • M Kabirnezhad
  • AC Kaboth
  • T Kajita
  • H Kakuno
  • J Kameda
  • SP Kasetti
  • Y Kataoka
  • Y Katayama
  • T Katori
  • M Kawaue
  • E Kearns
  • M Khabibullin
  • A Khotjantsev
  • T Kikawa
  • H Kikutani
  • S King
  • V Kiseeva
  • J Kisiel
  • T Kobata
  • H Kobayashi
  • T Kobayashi
  • L Koch
  • S Kodama
  • A Konaka
  • LL Kormos
  • Y Koshio
  • A Kostin
  • T Koto
  • K Kowalik
  • Y Kudenko
  • Y Kudo
  • S Kuribayashi
  • R Kurjata
  • T Kutter
  • M Kuze
  • M La Commara
  • L Labarga
  • K Lachner
  • J Lagoda
  • SM Lakshmi
  • M Lamers James
  • M Lamoureux
  • A Langella
  • J-F Laporte
  • D Last
  • N Latham
  • M Laveder
  • L Lavitola
  • M Lawe
  • Y Lee
  • C Lin
  • S-K Lin
  • RP Litchfield
  • SL Liu
  • W Li
  • A Longhin
  • KR Long
  • A Lopez Moreno
  • L Ludovici
  • X Lu
  • T Lux
  • LN Machado
  • L Magaletti
  • K Mahn
  • M Malek
  • M Mandal
  • S Manly
  • AD Marino
  • L Marti-Magro
  • DGR Martin
  • M Martini
  • JF Martin
  • T Maruyama
  • T Matsubara
  • V Matveev
  • C Mauger
  • K Mavrokoridis
  • E Mazzucato
  • N McCauley
  • J McElwee
  • KS McFarland
  • C McGrew
  • J McKean
  • A Mefodiev
  • GD Megias
  • P Mehta
  • L Mellet
  • C Metelko
  • M Mezzetto
  • E Miller
  • A Minamino
  • O Mineev
  • S Mine
  • M Miura
  • L Molina Bueno
  • S Moriyama
  • S Moriyama
  • P Morrison
  • Th A Mueller
  • D Munford
  • L Munteanu
  • K Nagai
  • Y Nagai
  • T Nakadaira
  • K Nakagiri
  • M Nakahata
  • Y Nakajima
  • A Nakamura
  • H Nakamura
  • K Nakamura
  • KD Nakamura
  • Y Nakano
  • S Nakayama
  • T Nakaya
  • K Nakayoshi
  • CER Naseby
  • TV Ngoc
  • VQ Nguyen
  • K Niewczas
  • S Nishimori
  • Y Nishimura
  • K Nishizaki
  • T Nosek
  • F Nova
  • P Novella
  • JC Nugent
  • HM O’Keeffe
  • L O’Sullivan
  • T Odagawa
  • T Ogawa
  • R Okada
  • W Okinaga
  • K Okumura
  • T Okusawa
  • N Ospina
  • RA Owen
  • Y Oyama
  • V Palladino
  • V Paolone
  • M Pari
  • J Parlone
  • S Parsa
  • J Pasternak
  • M Pavin
  • D Payne
  • GC Penn
  • D Pershey
  • L Pickering
  • C Pidcott
  • G Pintaudi
  • C Pistillo
  • B Popov
  • K Porwit
  • M Posiadala-Zezula
  • YS Prabhu
  • F Pupilli
  • B Quilain
  • T Radermacher
  • E Radicioni
  • B Radics
  • MA Ramírez
  • PN Ratoff
  • M Reh
  • C Riccio
  • E Rondio
  • S Roth
  • N Roy
  • A Rubbia
  • AC Ruggeri
  • CA Ruggles
  • A Rychter
  • K Sakashita
  • F Sánchez
  • G Santucci
  • CM Schloesser
  • K Scholberg
  • M Scott
  • Y Seiya
  • T Sekiguchi
  • H Sekiya
  • D Sgalaberna
  • A Shaikhiev
  • F Shaker
  • A Shaykina
  • M Shiozawa
  • W Shorrock
  • A Shvartsman
  • N Skrobova
  • K Skwarczynski
  • D Smyczek
  • M Smy
  • JT Sobczyk
  • H Sobel
  • FJP Soler
  • Y Sonoda
  • AJ Speers
  • R Spina
  • IA Suslov
  • S Suvorov
  • A Suzuki
  • SY Suzuki
  • Y Suzuki
  • AA Sztuc
  • M Tada
  • S Tairafune
  • S Takayasu
  • A Takeda
  • Y Takeuchi
  • K Takifuji
  • HK Tanaka
  • Y Tanihara
  • M Tani
  • A Teklu
  • VV Tereshchenko
  • N Teshima
  • N Thamm
  • LF Thompson
  • W Toki
  • C Touramanis
  • T Towstego
  • KM Tsui
  • T Tsukamoto
  • M Tzanov
  • Y Uchida
  • M Vagins
  • D Vargas
  • M Varghese
  • G Vasseur
  • C Vilela
  • E Villa
  • WGS Vinning
  • U Virginet
  • T Vladisavljevic
  • T Wachala
  • JG Walsh
  • Y Wang
  • L Wan
  • D Wark
  • MO Wascko
  • A Weber
  • R Wendell
  • MJ Wilking
  • C Wilkinson
  • JR Wilson
  • K Wood
  • C Wret
  • J Xia
  • Y-H Xu
  • K Yamamoto
  • T Yamamoto
  • C Yanagisawa
  • G Yang
  • T Yano
  • K Yasutome
  • N Yershov
  • U Yevarouskaya
  • M Yokoyama
  • Y Yoshimoto
  • N Yoshimura
  • M Yu
  • R Zaki
  • A Zalewska
  • J Zalipska
  • K Zaremba
  • G Zarnecki
  • X Zhao
  • T Zhu
  • M Ziembicki
  • ED Zimmerman
  • M Zito
  • S Zsoldos
DOI
10.1140/epjc/s10052-023-11819-x
eISSN
1434-6052
Ausgabe der Veröffentlichung
9
Zeitschrift
The European Physical Journal C
Sprache
en
Artikelnummer
782
Online publication date
2023
Status
Published online
Herausgeber
Springer Science and Business Media LLC
Herausgeber URL
http://dx.doi.org/10.1140/epjc/s10052-023-11819-x
Datum der Datenerfassung
2023
Titel
Measurements of neutrino oscillation parameters from the T2K experiment using $$3.6\times 10^{21}$$ protons on target
Ausgabe der Zeitschrift
83

Data source: Crossref

Abstract
The T2K experiment presents new measurements of neutrino oscillation parameters using 19.7(16.3)×1020 protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional 4.7×1020 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 sin2θ13 and the impact of priors on the δCP measurement. Both analyses prefer the normal mass ordering and upper octant of sin2θ23 with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on sin2θ13 from reactors, sin2θ23=0.561-0.032+0.021 using Feldman-Cousins corrected intervals, and Δm322=2.494-0.058+0.041×10-3eV2 using constant Δχ2 intervals. The CP-violating phase is constrained to δCP=-1.97-0.70+0.97 using Feldman-Cousins corrected intervals, and δCP=0,π is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than 2σ credible level using a flat prior in δCP, and just below 2σ using a flat prior in sinδCP. When the external constraint on sin2θ13 is removed, sin2θ13=28.0-6.5+2.8×10-3, in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.
Addresses
  • Kamioka Observatory, Institute for Cosmic Ray Research, University of Tokyo, Kamioka, Japan.
Autoren
  • K Abe
  • N Akhlaq
  • R Akutsu
  • A Ali
  • S Alonso Monsalve
  • C Alt
  • C Andreopoulos
  • M Antonova
  • S Aoki
  • T Arihara
  • Y Asada
  • Y Ashida
  • ET Atkin
  • M Barbi
  • GJ Barker
  • G Barr
  • D Barrow
  • M Batkiewicz-Kwasniak
  • F Bench
  • V Berardi
  • L Berns
  • S Bhadra
  • A Blanchet
  • A Blondel
  • S Bolognesi
  • T Bonus
  • S Bordoni
  • SB Boyd
  • A Bravar
  • C Bronner
  • S Bron
  • A Bubak
  • M Buizza Avanzini
  • JA Caballero
  • NF Calabria
  • S Cao
  • D Carabadjac
  • AJ Carter
  • SL Cartwright
  • MG Catanesi
  • A Cervera
  • J Chakrani
  • D Cherdack
  • PS Chong
  • G Christodoulou
  • A Chvirova
  • M Cicerchia
  • J Coleman
  • G Collazuol
  • L Cook
  • A Cudd
  • C Dalmazzone
  • T Daret
  • Yu I Davydov
  • A De Roeck
  • G De Rosa
  • T Dealtry
  • CC Delogu
  • C Densham
  • A Dergacheva
  • F Di Lodovico
  • S Dolan
  • D Douqa
  • TA Doyle
  • O Drapier
  • J Dumarchez
  • P Dunne
  • K Dygnarowicz
  • A Eguchi
  • S Emery-Schrenk
  • G Erofeev
  • A Ershova
  • G Eurin
  • D Fedorova
  • S Fedotov
  • M Feltre
  • AJ Finch
  • GA Fiorentini Aguirre
  • G Fiorillo
  • MD Fitton
  • JM Franco Patiño
  • M Friend
  • Y Fujii
  • Y Fukuda
  • K Fusshoeller
  • L Giannessi
  • C Giganti
  • V Glagolev
  • M Gonin
  • J González Rosa
  • EAG Goodman
  • A Gorin
  • M Grassi
  • M Guigue
  • DR Hadley
  • JT Haigh
  • P Hamacher-Baumann
  • DA Harris
  • M Hartz
  • T Hasegawa
  • S Hassani
  • NC Hastings
  • Y Hayato
  • D Henaff
  • A Hiramoto
  • M Hogan
  • J Holeczek
  • A Holin
  • T Holvey
  • NT Hong Van
  • T Honjo
  • F Iacob
  • AK Ichikawa
  • M Ikeda
  • T Ishida
  • M Ishitsuka
  • HT Israel
  • K Iwamoto
  • A Izmaylov
  • N Izumi
  • M Jakkapu
  • B Jamieson
  • SJ Jenkins
  • C Jesús-Valls
  • JJ Jiang
  • P Jonsson
  • S Joshi
  • CK Jung
  • PB Jurj
  • M Kabirnezhad
  • AC Kaboth
  • T Kajita
  • H Kakuno
  • J Kameda
  • SP Kasetti
  • Y Kataoka
  • Y Katayama
  • T Katori
  • M Kawaue
  • E Kearns
  • M Khabibullin
  • A Khotjantsev
  • T Kikawa
  • H Kikutani
  • S King
  • V Kiseeva
  • J Kisiel
  • T Kobata
  • H Kobayashi
  • T Kobayashi
  • L Koch
  • S Kodama
  • A Konaka
  • LL Kormos
  • Y Koshio
  • A Kostin
  • T Koto
  • K Kowalik
  • Y Kudenko
  • Y Kudo
  • S Kuribayashi
  • R Kurjata
  • T Kutter
  • M Kuze
  • M La Commara
  • L Labarga
  • K Lachner
  • J Lagoda
  • SM Lakshmi
  • M Lamers James
  • M Lamoureux
  • A Langella
  • J-F Laporte
  • D Last
  • N Latham
  • M Laveder
  • L Lavitola
  • M Lawe
  • Y Lee
  • C Lin
  • S-K Lin
  • RP Litchfield
  • SL Liu
  • W Li
  • A Longhin
  • KR Long
  • A Lopez Moreno
  • L Ludovici
  • X Lu
  • T Lux
  • LN Machado
  • L Magaletti
  • K Mahn
  • M Malek
  • M Mandal
  • S Manly
  • AD Marino
  • L Marti-Magro
  • DGR Martin
  • M Martini
  • JF Martin
  • T Maruyama
  • T Matsubara
  • V Matveev
  • C Mauger
  • K Mavrokoridis
  • E Mazzucato
  • N McCauley
  • J McElwee
  • KS McFarland
  • C McGrew
  • J McKean
  • A Mefodiev
  • GD Megias
  • P Mehta
  • L Mellet
  • C Metelko
  • M Mezzetto
  • E Miller
  • A Minamino
  • O Mineev
  • S Mine
  • M Miura
  • L Molina Bueno
  • S Moriyama
  • S Moriyama
  • P Morrison
  • Th A Mueller
  • D Munford
  • L Munteanu
  • K Nagai
  • Y Nagai
  • T Nakadaira
  • K Nakagiri
  • M Nakahata
  • Y Nakajima
  • A Nakamura
  • H Nakamura
  • K Nakamura
  • KD Nakamura
  • Y Nakano
  • S Nakayama
  • T Nakaya
  • K Nakayoshi
  • CER Naseby
  • TV Ngoc
  • VQ Nguyen
  • K Niewczas
  • S Nishimori
  • Y Nishimura
  • K Nishizaki
  • T Nosek
  • F Nova
  • P Novella
  • JC Nugent
  • HM O'Keeffe
  • L O'Sullivan
  • T Odagawa
  • T Ogawa
  • R Okada
  • W Okinaga
  • K Okumura
  • T Okusawa
  • N Ospina
  • RA Owen
  • Y Oyama
  • V Palladino
  • V Paolone
  • M Pari
  • J Parlone
  • S Parsa
  • J Pasternak
  • M Pavin
  • D Payne
  • GC Penn
  • D Pershey
  • L Pickering
  • C Pidcott
  • G Pintaudi
  • C Pistillo
  • B Popov
  • K Porwit
  • M Posiadala-Zezula
  • YS Prabhu
  • F Pupilli
  • B Quilain
  • T Radermacher
  • E Radicioni
  • B Radics
  • MA Ramírez
  • PN Ratoff
  • M Reh
  • C Riccio
  • E Rondio
  • S Roth
  • N Roy
  • A Rubbia
  • AC Ruggeri
  • CA Ruggles
  • A Rychter
  • K Sakashita
  • F Sánchez
  • G Santucci
  • CM Schloesser
  • K Scholberg
  • M Scott
  • Y Seiya
  • T Sekiguchi
  • H Sekiya
  • D Sgalaberna
  • A Shaikhiev
  • F Shaker
  • A Shaykina
  • M Shiozawa
  • W Shorrock
  • A Shvartsman
  • N Skrobova
  • K Skwarczynski
  • D Smyczek
  • M Smy
  • JT Sobczyk
  • H Sobel
  • FJP Soler
  • Y Sonoda
  • AJ Speers
  • R Spina
  • IA Suslov
  • S Suvorov
  • A Suzuki
  • SY Suzuki
  • Y Suzuki
  • AA Sztuc
  • M Tada
  • S Tairafune
  • S Takayasu
  • A Takeda
  • Y Takeuchi
  • K Takifuji
  • HK Tanaka
  • Y Tanihara
  • M Tani
  • A Teklu
  • VV Tereshchenko
  • N Teshima
  • N Thamm
  • LF Thompson
  • W Toki
  • C Touramanis
  • T Towstego
  • KM Tsui
  • T Tsukamoto
  • M Tzanov
  • Y Uchida
  • M Vagins
  • D Vargas
  • M Varghese
  • G Vasseur
  • C Vilela
  • E Villa
  • WGS Vinning
  • U Virginet
  • T Vladisavljevic
  • T Wachala
  • JG Walsh
  • Y Wang
  • L Wan
  • D Wark
  • MO Wascko
  • A Weber
  • R Wendell
  • MJ Wilking
  • C Wilkinson
  • JR Wilson
  • K Wood
  • C Wret
  • J Xia
  • Y-H Xu
  • K Yamamoto
  • T Yamamoto
  • C Yanagisawa
  • G Yang
  • T Yano
  • K Yasutome
  • N Yershov
  • U Yevarouskaya
  • M Yokoyama
  • Y Yoshimoto
  • N Yoshimura
  • M Yu
  • R Zaki
  • A Zalewska
  • J Zalipska
  • K Zaremba
  • G Zarnecki
  • X Zhao
  • T Zhu
  • M Ziembicki
  • ED Zimmerman
  • M Zito
  • S Zsoldos
  • T2K Collaboration
DOI
10.1140/epjc/s10052-023-11819-x
eISSN
1434-6052
Externe Identifier
  • PubMed Identifier: 37680254
  • PubMed Central ID: PMC10480298
Funding acknowledgements
  • Swiss National Science Foundation: 20FL21_186178I
  • ‘la Caixa’: ID 100010434, fellowship code LCF/BQ/IN17/11620050
  • Horizon 2020 Framework Programme: RISE-GA872549-SK2HK
  • Deutsche Forschungsgemeinschaft: RO 3625/2
  • Russian Science Foundation: RSF19-12-00325
  • European Regional Development Fund:
  • Science and Technology Facilities Council:
  • Japan Society for the Promotion of Science: JP16H06288
  • Japan Society for the Promotion of Science: JP20H00149
  • Japan Society for the Promotion of Science: JP20H00162
  • Medical Research Council: MR/T041323/1
  • Ministerio de Ciencia e Innovación: PID2019-107564GB-I00
  • Science and Technology Facilities Council: ST/S000739/1
  • Science and Technology Facilities Council: ST/W000571/1
  • Staatssekretariat für Bildung, Forschung und Innovation:
  • UK Research and Innovation:
  • Swiss National Science Foundation: 185012
  • Japan Society for the Promotion of Science: JP18H05537
  • Russian Science Foundation: RSF22-12-00358
  • Centres de Recerca de Catalunya:
  • Swiss National Science Foundation: 200020
  • Swiss National Science Foundation: 200020_188533
  • Japan Society for the Promotion of Science: JP18H03701
  • Japan Society for the Promotion of Science: JP19J22258
  • Japan Society for the Promotion of Science: JP19J22440
  • SNF Eccellenza: PCEFP2_203261
  • Science and Technology Facilities Council: ST/S000933/1
  • Science and Technology Facilities Council: ST/X006042/1
  • Instituto Nazionale di Fisica Nucleare:
  • Ministry of Science and Higher Education of the Russian Federation: 075-15-2020-778
  • Swiss National Science Foundation: 200021_185012
  • Agence Nationale de la Recherche: ANR-19-CE31-0001
  • Science and Technology Facilities Council: ST/W000636/1
  • Science and Technology Facilities Council: ST/W004917/1
  • Ministry of Education, Culture, Sports, Science and Technology:
  • Swiss National Science Foundation: 200021
  • Horizon 2020 Framework Programme: 713673
  • Horizon 2020 Framework Programme: 754496
  • Ministry of Education and Science, Poland: DIR/WK/2017/05
  • Japan Society for the Promotion of Science: JPJSBP120209601
  • Ministerio de Ciencia e Innovación: SEV-2016-0588
  • Science and Technology Facilities Council: ST/W000628/1
  • Narodowe Centrum Nauki: UMO-2018/30/E/ST2/00441
  • Canadian Network for Research and Innovation in Machining Technology, Natural Sciences and Engineering Research Council of Canada:
  • Centre National de la Recherche Scientifique:
  • National Research Council Canada:
  • Royal Society:
  • Swiss National Science Foundation: 188533
  • Japan Society for the Promotion of Science: JP19J01119
  • Japan Society for the Promotion of Science: JP20J20304
  • Japan Society for the Promotion of Science: JPJSBP120204806
  • Ministerio de Ciencia e Innovación: PGC2018-099388-BI00
  • Horizon 2020 Framework Programme: RISE-GA822070-JENNIFER2
  • Science and Technology Facilities Council: ST/V00204X/1
  • Canada Foundation for Innovation:
  • European Research Council:
  • U.S. Department of Energy:
  • Swiss National Science Foundation: 203261
  • Japan Society for the Promotion of Science: JP18K03682
  • Science and Technology Facilities Council: ST/W000660/1
  • Commissariat à l’Énergie Atomique et aux Énergies Alternatives:
Open access
true
ISSN
1434-6044
Ausgabe der Veröffentlichung
9
Zeitschrift
The European physical journal. C, Particles and fields
Schlüsselwörter
  • T2K Collaboration
Sprache
eng
Medium
Print-Electronic
Online publication date
2023
Open access status
Open Access
Paginierung
782
Datum der Veröffentlichung
2023
Status
Published
Publisher licence
CC BY
Datum der Datenerfassung
2023
Titel
Measurements of neutrino oscillation parameters from the T2K experiment using 3.6×1021 protons on target.
Sub types
  • research-article
  • Journal Article
Ausgabe der Zeitschrift
83

Files

https://link.springer.com/content/pdf/10.1140/epjc/s10052-023-11819-x.pdf https://europepmc.org/articles/PMC10480298?pdf=render

Data source: Europe PubMed Central

Abstract
The T2K experiment presents new measurements of neutrino oscillation parameters using 19.7(16.3)×1020 protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional 4.7×1020 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 sin2θ13 and the impact of priors on the δCP measurement. Both analyses prefer the normal mass ordering and upper octant of sin2θ23 with a nearly maximally CP-violating phase. Assuming the normal ordering and using the constraint on sin2θ13 from reactors, sin2θ23=0.561-0.032+0.021 using Feldman-Cousins corrected intervals, and Δm322=2.494-0.058+0.041×10-3eV2 using constant Δχ2 intervals. The CP-violating phase is constrained to δCP=-1.97-0.70+0.97 using Feldman-Cousins corrected intervals, and δCP=0,π is excluded at more than 90% confidence level. A Jarlskog invariant of zero is excluded at more than 2σ credible level using a flat prior in δCP, and just below 2σ using a flat prior in sinδCP. When the external constraint on sin2θ13 is removed, sin2θ13=28.0-6.5+2.8×10-3, in agreement with measurements from reactor experiments. These results are consistent with previous T2K analyses.
Date of acceptance
2023
Autoren
  • K Abe
  • N Akhlaq
  • R Akutsu
  • A Ali
  • S Alonso Monsalve
  • C Alt
  • C Andreopoulos
  • M Antonova
  • S Aoki
  • T Arihara
  • Y Asada
  • Y Ashida
  • ET Atkin
  • M Barbi
  • GJ Barker
  • G Barr
  • D Barrow
  • M Batkiewicz-Kwasniak
  • F Bench
  • V Berardi
  • L Berns
  • S Bhadra
  • A Blanchet
  • A Blondel
  • S Bolognesi
  • T Bonus
  • S Bordoni
  • SB Boyd
  • A Bravar
  • C Bronner
  • S Bron
  • A Bubak
  • M Buizza Avanzini
  • JA Caballero
  • NF Calabria
  • S Cao
  • D Carabadjac
  • AJ Carter
  • SL Cartwright
  • MG Catanesi
  • A Cervera
  • J Chakrani
  • D Cherdack
  • PS Chong
  • G Christodoulou
  • A Chvirova
  • M Cicerchia
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  • T2K Collaboration
Autoren-URL
https://www.ncbi.nlm.nih.gov/pubmed/37680254
DOI
10.1140/epjc/s10052-023-11819-x
Externe Identifier
  • PubMed Central ID: PMC10480298
Funding acknowledgements
  • Medical Research Council: MR/T041323/1
ISSN
1434-6044
Ausgabe der Veröffentlichung
9
Zeitschrift
Eur Phys J C Part Fields
Sprache
eng
Country
France
Paginierung
782
PII
11819
Datum der Veröffentlichung
2023
Status
Published
Titel
Measurements of neutrino oscillation parameters from the T2K experiment using 3.6×1021 protons on target.
Sub types
  • Journal Article
Ausgabe der Zeitschrift
83

Data source: PubMed

Beziehungen:
Has preprint
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