Measurement of Coherent π^{+} Production in Low Energy Neutrino-Carbon Scattering.

نویسندگان

  • K Abe
  • C Andreopoulos
  • M Antonova
  • S Aoki
  • A Ariga
  • S Assylbekov
  • D Autiero
  • S Ban
  • M Barbi
  • G J Barker
  • G Barr
  • P Bartet-Friburg
  • M Batkiewicz
  • F Bay
  • V Berardi
  • S Berkman
  • S Bhadra
  • A Blondel
  • S Bolognesi
  • S Bordoni
  • S B Boyd
  • D Brailsford
  • A Bravar
  • C Bronner
  • M Buizza Avanzini
  • R G Calland
  • T Campbell
  • S Cao
  • J Caravaca Rodríguez
  • S L Cartwright
  • R Castillo
  • M G Catanesi
  • A Cervera
  • D Cherdack
  • N Chikuma
  • G Christodoulou
  • A Clifton
  • J Coleman
  • G Collazuol
  • D Coplowe
  • L Cremonesi
  • A Dabrowska
  • G De Rosa
  • T Dealtry
  • P F Denner
  • S R Dennis
  • C Densham
  • D Dewhurst
  • F Di Lodovico
  • S Di Luise
  • S Dolan
  • O Drapier
  • K E Duffy
  • J Dumarchez
  • S Dytman
  • M Dziewiecki
  • S Emery-Schrenk
  • A Ereditato
  • T Feusels
  • A J Finch
  • G A Fiorentini
  • M Friend
  • Y Fujii
  • D Fukuda
  • Y Fukuda
  • A P Furmanski
  • V Galymov
  • A Garcia
  • S G Giffin
  • C Giganti
  • F Gizzarelli
  • M Gonin
  • N Grant
  • D R Hadley
  • L Haegel
  • M D Haigh
  • P Hamilton
  • D Hansen
  • J Harada
  • T Hara
  • M Hartz
  • T Hasegawa
  • N C Hastings
  • T Hayashino
  • Y Hayato
  • R L Helmer
  • M Hierholzer
  • A Hillairet
  • A Himmel
  • T Hiraki
  • S Hirota
  • M Hogan
  • J Holeczek
  • S Horikawa
  • F Hosomi
  • K Huang
  • A K Ichikawa
  • K Ieki
  • M Ikeda
  • J Imber
  • J Insler
  • R A Intonti
  • T J Irvine
  • T Ishida
  • T Ishii
  • E Iwai
  • K Iwamoto
  • A Izmaylov
  • A Jacob
  • B Jamieson
  • M Jiang
  • S Johnson
  • J H Jo
  • P Jonsson
  • C K Jung
  • M Kabirnezhad
  • A C Kaboth
  • T Kajita
  • H Kakuno
  • J Kameda
  • D Karlen
  • I Karpikov
  • T Katori
  • E Kearns
  • M Khabibullin
  • A Khotjantsev
  • D Kielczewska
  • T Kikawa
  • H Kim
  • J Kim
  • S King
  • J Kisiel
  • A Knight
  • A Knox
  • T Kobayashi
  • L Koch
  • T Koga
  • A Konaka
  • K Kondo
  • A Kopylov
  • L L Kormos
  • A Korzenev
  • Y Koshio
  • W Kropp
  • Y Kudenko
  • R Kurjata
  • T Kutter
  • J Lagoda
  • I Lamont
  • E Larkin
  • P Lasorak
  • M Laveder
  • M Lawe
  • M Lazos
  • T Lindner
  • Z J Liptak
  • R P Litchfield
  • X Li
  • A Longhin
  • J P Lopez
  • L Ludovici
  • X Lu
  • L Magaletti
  • K Mahn
  • M Malek
  • S Manly
  • A D Marino
  • J Marteau
  • J F Martin
  • P Martins
  • S Martynenko
  • T Maruyama
  • V Matveev
  • K Mavrokoridis
  • W Y Ma
  • E Mazzucato
  • M McCarthy
  • N McCauley
  • K S McFarland
  • C McGrew
  • A Mefodiev
  • C Metelko
  • M Mezzetto
  • P Mijakowski
  • A Minamino
  • O Mineev
  • S Mine
  • A Missert
  • M Miura
  • S Moriyama
  • Th A Mueller
  • S Murphy
  • J Myslik
  • T Nakadaira
  • M Nakahata
  • K G Nakamura
  • K Nakamura
  • K D Nakamura
  • S Nakayama
  • T Nakaya
  • K Nakayoshi
  • C Nantais
  • C Nielsen
  • M Nirkko
  • K Nishikawa
  • Y Nishimura
  • P Novella
  • J Nowak
  • H M O'Keeffe
  • R Ohta
  • K Okumura
  • T Okusawa
  • W Oryszczak
  • S M Oser
  • T Ovsyannikova
  • R A Owen
  • Y Oyama
  • V Palladino
  • J L Palomino
  • V Paolone
  • N D Patel
  • M Pavin
  • D Payne
  • J D Perkin
  • Y Petrov
  • L Pickard
  • L Pickering
  • E S Pinzon Guerra
  • C Pistillo
  • B Popov
  • M Posiadala-Zezula
  • J-M Poutissou
  • R Poutissou
  • P Przewlocki
  • B Quilain
  • T Radermacher
  • E Radicioni
  • P N Ratoff
  • M Ravonel
  • M A M Rayner
  • A Redij
  • E Reinherz-Aronis
  • C Riccio
  • P Rojas
  • E Rondio
  • S Roth
  • A Rubbia
  • A Rychter
  • R Sacco
  • K Sakashita
  • F Sánchez
  • F Sato
  • E Scantamburlo
  • K Scholberg
  • S Schoppmann
  • J Schwehr
  • M Scott
  • Y Seiya
  • T Sekiguchi
  • H Sekiya
  • D Sgalaberna
  • R Shah
  • A Shaikhiev
  • F Shaker
  • D Shaw
  • M Shiozawa
  • T Shirahige
  • S Short
  • M Smy
  • J T Sobczyk
  • H Sobel
  • M Sorel
  • L Southwell
  • P Stamoulis
  • J Steinmann
  • T Stewart
  • P Stowell
  • Y Suda
  • S Suvorov
  • A Suzuki
  • K Suzuki
  • S Y Suzuki
  • Y Suzuki
  • R Tacik
  • M Tada
  • S Takahashi
  • A Takeda
  • Y Takeuchi
  • H K Tanaka
  • H A Tanaka
  • D Terhorst
  • R Terri
  • T Thakore
  • L F Thompson
  • S Tobayama
  • W Toki
  • T Tomura
  • C Touramanis
  • T Tsukamoto
  • M Tzanov
  • Y Uchida
  • A Vacheret
  • M Vagins
  • Z Vallari
  • G Vasseur
  • T Wachala
  • K Wakamatsu
  • C W Walter
  • D Wark
  • W Warzycha
  • M O Wascko
  • A Weber
  • R Wendell
  • R J Wilkes
  • M J Wilking
  • C Wilkinson
  • J R Wilson
  • R J Wilson
  • Y Yamada
  • K Yamamoto
  • M Yamamoto
  • C Yanagisawa
  • T Yano
  • S Yen
  • N Yershov
  • M Yokoyama
  • J Yoo
  • K Yoshida
  • T Yuan
  • M Yu
  • A Zalewska
  • J Zalipska
  • L Zambelli
  • K Zaremba
  • M Ziembicki
  • E D Zimmerman
  • M Zito
  • J Żmuda
چکیده

We report the first measurement of the flux-averaged cross section for charged current coherent π^{+} production on carbon for neutrino energies less than 1.5 GeV, and with a restriction on the final state phase space volume in the T2K near detector, ND280. Comparisons are made with predictions from the Rein-Sehgal coherent production model and the model by Alvarez-Ruso et al., the latter representing the first implementation of an instance of the new class of microscopic coherent models in a neutrino interaction Monte Carlo event generator. We observe a clear event excess above background, disagreeing with the null results reported by K2K and SciBooNE in a similar neutrino energy region. The measured flux-averaged cross sections are below those predicted by both the Rein-Sehgal and Alvarez-Ruso et al. MODELS

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

PCAC and coherent pion production by neutrinos

Abstract. Coherent π and π production in low energy neutrino reactions is discussed in the framework of the partially conserved axial vector current theory (PCAC). The role of lepton mass effects in suppressing the π production is discussed. Instead of using models of pion nucleus scattering, the available data on pion carbon scattering are implemented for an analysis of the PCAC prediction. Ou...

متن کامل

First Observation of Coherent π 0 Production in Neutrino Nucleus Interactions with E ν < 2 GeV

The MiniBooNE experiment at Fermilab has amassed the largest sample to date of πs produced in neutral current (NC) neutrino-nucleus interactions at low energy. This paper reports a measurement of the momentum distribution of πs produced in mineral oil (CH2) and the first observation of coherent π 0 production below 2 GeV. In the forward direction, the yield of events observed above the expectat...

متن کامل

Measurement of coherent production of π(±) in neutrino and antineutrino beams on carbon from Eν of 1.5 to 20 GeV.

Neutrino-induced coherent charged pion production on nuclei νμA→μ(±)π(∓)A is a rare, inelastic interaction in which a small squared four-momentum |t| is transferred to the recoil nucleus, leaving it intact in the reaction. In the scintillator tracker of MINERvA, we remove events with evidence of particles from nuclear breakup and reconstruct |t| from the final-state pion and muon. We select low...

متن کامل

Search for neutrino charged current coherent pion production at SciBooNE

Abstract. SciBooNE is a neutrino experiment measuring neutrino cross sections on carbon in the one GeV region. We have performed a search for charged current coherent pion production from muon neutrinos scattering on carbon, νμ 12C → μ−12Cπ+. No evidence for coherent pion production is observed. We set 90% confidence level upper limits on the cross section ratio of charged current coherent pion...

متن کامل

PCAC and the Deficit of Forward Muons in π Production by Neutrinos

The K2K experiment, using a fine-grained detector in a neutrino beam of energy < E > ∼ 1.3GeV has observed two-track events that can be interpreted as a coherent reaction νμ + N → μ − + N + π (N = C) or an incoherent process νμ + (p, n) → μ − + π + (p, n), the final nucleon being unobserved. The data show a significant deficit of forward-going muons in the interval Q . 0.1GeV, where a sizeable ...

متن کامل

Charged Current Single Pion Cross Section Measurement at MiniBooNE

Charged current single pion (CC1π) production has been studied since the advent of high energy neutrino beams, but the cross section around 1 GeV energy is still not well understood. Also, many of the data that do exist come from hydrogen and deuterium targets, so there is still a significant need to study nuclear effects in this process. Figure 1 [3] shows a comparison of the CC1π measurements...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:
  • Physical review letters

دوره 117 19  شماره 

صفحات  -

تاریخ انتشار 2016